continua.cc

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/* Copyright (C) 2001 Thomas Kuhn    <tkuhn@uni-bremen.de>
                      Stefan Buehler <sbuehler@uni-bremen.de>

   This program is free software; you can redistribute it and/or modify it
   under the terms of the GNU General Public License as published by the
   Free Software Foundation; either version 2, or (at your option) any
   later version.

   This program is distributed in the hope that it will be useful,
   but WITHOUT ANY WARRANTY; without even the implied warranty of
   MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
   GNU General Public License for more details.

   You should have received a copy of the GNU General Public License
   along with this program; if not, write to the Free Software
   Foundation, Inc., 59 Temple Place - Suite 330, Boston, MA 02111-1307,
   USA. */

#include <cmath>
#include "arts.h"
#include "matpackI.h"
#include "array.h"
#include "absorption.h"
#include "messages.h"
#include "continua.h"

// #################################################################################

// global constants as defined in constants.cc

extern const Numeric EULER_NUMBER;
extern const Numeric LOG10_EULER_NUMBER;
extern const Numeric NAT_LOG_TEN;
extern const Numeric PI;
extern const Numeric SPEED_OF_LIGHT;

// numerical constants specific defined for the file continua.cc

// conversion from neper to decibel:
const Numeric Np_to_dB  = (10.000000 * LOG10_EULER_NUMBER); // [dB/Np]
// conversion from decibel to neper:
const Numeric dB_to_Np  = (1.000000 / Np_to_dB);            // [Np/dB]
// conversion from GHz to Hz:
const Numeric GHz_to_Hz = 1.000000e9;                       // [Hz/GHz]
// conversion from Hz to GHz:
const Numeric Hz_to_GHz = 1.000000e-9;                      // [GHz/Hz]
// conversion from kPa to Pa:
const Numeric kPa_to_Pa = 1.000000e3;                       // [kPa/Pa]
// conversion from Pa to kPa:
const Numeric Pa_to_kPa = 1.000000e-3;                      // [Pa/kPa]
// conversion from hPa to Pa (hPa = mbar):
const Numeric hPa_to_Pa = 1.000000e2;                       // [hPa/Pa]
// conversion from Pa to hPa (hPa = mbar):
const Numeric Pa_to_hPa = 1.000000e-2;                      // [Pa/hPa]

// MPM pre-factor for unit setting:
const Numeric dB_m_Hz   = 0.1820427855916028e-06; // [dB/m/Hz]   (4 * pi / c) * 10 * log(e)
const Numeric dB_km_GHz = 0.1820427855916028e+06; // [dB/km/GHz] (4 * pi / c) * 10 * log(e)


// absorption unit conversions

// conversion from dB/km to Np/km for absorption units:
const Numeric dB_km_to_Np_km = dB_to_Np;
// conversion from dB/km to Np/m for absorption units:
const Numeric dB_km_to_Np_m  = (1.00000e-3 / (10.0 * LOG10_EULER_NUMBER));
// conversion from dB/km to 1/m for absorption units:
const Numeric dB_km_to_1_m   = (1.00000e-3 / (10.0 * LOG10_EULER_NUMBER));


// lower limit for absorption calculation due to underflow error:

const Numeric VMRCalcLimit = 1.000e-25;

// #################################################################################
// ############################## WATER VAPOR MODELS ###############################
// #################################################################################
//
void MPM87H2OAbsModel( MatrixView        xsec,
                       const Numeric     CCin,       // continuum scale factor 
                       const Numeric     CLin,       // line strength scale factor
                       const Numeric     CWin,       // line broadening scale factor
                       const String&     model,
                       ConstVectorView   f_mono,
                       ConstVectorView   p_abs,
                       ConstVectorView   t_abs,
                       ConstVectorView   vmr )
{
  //
  // Coefficients are from Liebe, Radio Science, 20(5), 1985, 1069
  //         0           1        2       3      
  //         f0          b1       b2      b3     
  //        [GHz]     [kHz/kPa]   [1]   [GHz/kPa]
  const Numeric mpm87[30][4] = { 
    {    22.235080,    0.1090,  2.143,   27.84e-3},
    {    67.813960,    0.0011,  8.730,   27.60e-3},
    {   119.995940,    0.0007,  8.347,   27.00e-3},
    {   183.310117,    2.3000,  0.653,   31.64e-3},
    {   321.225644,    0.0464,  6.156,   21.40e-3},
    {   325.152919,    1.5400,  1.515,   29.70e-3},
    {   336.187000,    0.0010,  9.802,   26.50e-3},
    {   380.197372,   11.9000,  1.018,   30.36e-3},
    {   390.134508,    0.0044,  7.318,   19.00e-3},
    {   437.346667,    0.0637,  5.015,   13.70e-3},
    {   439.150812,    0.9210,  3.561,   16.40e-3},
    {   443.018295,    0.1940,  5.015,   14.40e-3},
    {   448.001075,   10.6000,  1.370,   23.80e-3},
    {   470.888947,    0.3300,  3.561,   18.20e-3},
    {   474.689127,    1.2800,  2.342,   19.80e-3},
    {   488.491133,    0.2530,  2.814,   24.90e-3},
    {   503.568532,    0.0374,  6.693,   11.50e-3},
    {   504.482692,    0.0125,  6.693,   11.90e-3},
    {   556.936002,  510.0000,  0.114,   30.00e-3},
    {   620.700807,    5.0900,  2.150,   22.30e-3},
    {   658.006500,    0.2740,  7.767,   30.00e-3},
    {   752.033227,  250.0000,  0.336,   28.60e-3},
    {   841.073593,    0.0130,  8.113,   14.10e-3},
    {   859.865000,    0.1330,  7.989,   28.60e-3},
    {   899.407000,    0.0550,  7.845,   28.60e-3},
    {   902.555000,    0.0380,  8.360,   26.40e-3},
    {   906.205524,    0.1830,  5.039,   23.40e-3},
    {   916.171582,    8.5600,  1.369,   25.30e-3},
    {   970.315022,    9.1600,  1.842,   24.00e-3},
    {   987.926764,  138.0000,  0.178,   28.60e-3}};

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the MPM87 model (Radio Science, 20(5), 1985, 1069):
  const Numeric CC_MPM87 = 1.00000;
  const Numeric CL_MPM87 = 1.00000;
  const Numeric CW_MPM87 = 1.00000;
  // ---------------------------------------------------------------------------------------


  // select the parameter set (!!model dominates values!!):
  Numeric CC, CL, CW;
  if ( model == "MPM87" )
    {
      CC = CC_MPM87;
      CL = CL_MPM87;
      CW = CW_MPM87;
    }
  else if ( model == "MPM87Lines" )
    {
      CC = 0.000;
      CL = CL_MPM87;
      CW = CW_MPM87;
    }
  else if ( model == "MPM87Continuum" )
    {
      CC = CC_MPM87;
      CL = 0.000;
      CW = 0.000;
    }
  else if ( model == "user" )
    {
      CC = CCin;
      CL = CLin;
      CW = CWin;
    }
  else
    {
      ostringstream os;
      os << "H2O-MPM87: ERROR! Wrong model values given.\n"
         << "Valid models are: 'MPM87', 'MPM87Lines', 'MPM87Continuum', and 'user'" << '\n';
      throw runtime_error(os.str());
    }
  out3  << "H2O-MPM87: (model=" << model << ") parameter values in use:\n" 
        << " CC = " << CC << "\n"
        << " CL = " << CL << "\n"
        << " CW = " << CW << "\n";
  
  
  // number of lines of liebe line catalog (30 lines)
  const Index i_first = 0;
  const Index i_last  = 29;
  
  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );

  // Loop pressure/temperature (pressure in [hPa] therefore the factor 0.01)
  for ( Index i=0; i<n_p; ++i )
    {
      // here the total pressure is not multiplied by the H2O vmr for the 
      // P_H2O calculation because we calculate xsec and not abs: abs = vmr * xsec
      Numeric pwv_dummy = Pa_to_kPa * p_abs[i];
      // relative inverse temperature [1]
      Numeric theta = (300.0 / t_abs[i]);
      // H2O partial pressure [kPa]
      Numeric pwv   = Pa_to_kPa * p_abs[i] * vmr[i];
      // dry air partial pressure [kPa]
      Numeric pda   = (Pa_to_kPa * p_abs[i]) - pwv;
      // H2O continuum absorption [dB/km/GHz2] like in the original MPM87
      Numeric Nppc  = CC * pwv_dummy * pow(theta, (Numeric)3.0) * 1.000e-5
        * ( (0.113 * pda) + (3.57 * pwv * pow(theta, (Numeric)7.8)) );

      // Loop over input frequency
      for ( Index s=0; s<n_f; ++s )
        {
          // input frequency in [GHz]
          Numeric ff   = f_mono[s] * Hz_to_GHz; 
          // H2O line contribution at position f
          Numeric Nppl = 0.000;
          
          // Loop over MPM89 H2O spectral lines
          for ( Index l = i_first; l <= i_last; ++l )
            {
              // line strength [kHz]
              Numeric strength = CL * pwv_dummy * mpm87[l][1]
                * pow(theta,(Numeric)3.5) * exp(mpm87[l][2]*(1.000-theta));
              // line broadening parameter [GHz]
              Numeric gam      = CW * mpm87[l][3] * 
                ( (4.80 * pwv * pow(theta, (Numeric)1.1)) + 
                  (       pda * pow(theta, (Numeric)0.6)) );
              // effective line width with Doppler broadening [GHz]
              // gam              = sqrt(gam*gam + (2.14e-12 * mpm87[l][0] * mpm87[l][0] / theta));
              // H2O line absorption [dB/km/GHz] like in the original MPM87
              Nppl            += strength * MPMLineShapeFunction(gam, mpm87[l][0], ff); 
            }
          // xsec = abs/vmr [1/m] but MPM87 is in [dB/km] --> conversion necessary
          xsec(s,i)  += dB_km_to_1_m * 0.1820 * ff * ( Nppl + (Nppc * ff) );
        }
    }
  return;
}
//
// #################################################################################
//
void MPM89H2OAbsModel( MatrixView        xsec,
                       const Numeric     CCin,       // continuum scale factor 
                       const Numeric     CLin,       // line strength scale factor
                       const Numeric     CWin,       // line broadening scale factor
                       const String&     model,     // model
                       ConstVectorView   f_mono,
                       ConstVectorView   p_abs,
                       ConstVectorView   t_abs,
                       ConstVectorView   vmr )
{
  //
  // Coefficients are from Liebe, Int. J. Infrared and Millimeter Waves, 10(6), 1989, 631
  //         0           1        2       3        4      5      6
  //         f0          b1       b2      b3       b4     b5     b6
  //        [GHz]     [kHz/kPa]   [1]   [MHz/kPa]  [1]    [1]    [1]
  const Numeric mpm89[30][7] = { 
    {    22.235080,    0.1090,  2.143,   28.11,   0.69,  4.80,  1.00},
    {    67.813960,    0.0011,  8.735,   28.58,   0.69,  4.93,  0.82},
    {   119.995940,    0.0007,  8.356,   29.48,   0.70,  4.78,  0.79},
    {   183.310074,    2.3000,  0.668,   28.13,   0.64,  5.30,  0.85},
    {   321.225644,    0.0464,  6.181,   23.03,   0.67,  4.69,  0.54},
    {   325.152919,    1.5400,  1.540,   27.83,   0.68,  4.85,  0.74},
    {   336.187000,    0.0010,  9.829,   26.93,   0.69,  4.74,  0.61},
    {   380.197372,   11.9000,  1.048,   28.73,   0.69,  5.38,  0.84},
    {   390.134508,    0.0044,  7.350,   21.52,   0.63,  4.81,  0.55},
    {   437.346667,    0.0637,  5.050,   18.45,   0.60,  4.23,  0.48},
    {   439.150812,    0.9210,  3.596,   21.00,   0.63,  4.29,  0.52},
    {   443.018295,    0.1940,  5.050,   18.60,   0.60,  4.23,  0.50},
    {   448.001075,   10.6000,  1.405,   26.32,   0.66,  4.84,  0.67},
    {   470.888947,    0.3300,  3.599,   21.52,   0.66,  4.57,  0.65},
    {   474.689127,    1.2800,  2.381,   23.55,   0.65,  4.65,  0.64},
    {   488.491133,    0.2530,  2.853,   26.02,   0.69,  5.04,  0.72},
    {   503.568532,    0.0374,  6.733,   16.12,   0.61,  3.98,  0.43},
    {   504.482692,    0.0125,  6.733,   16.12,   0.61,  4.01,  0.45},
    {   556.936002,  510.0000,  0.159,   32.10,   0.69,  4.11,  1.00},
    {   620.700807,    5.0900,  2.200,   24.38,   0.71,  4.68,  0.68},
    {   658.006500,    0.2740,  7.820,   32.10,   0.69,  4.14,  1.00},
    {   752.033227,  250.0000,  0.396,   30.60,   0.68,  4.09,  0.84},
    {   841.073593,    0.0130,  8.180,   15.90,   0.33,  5.76,  0.45},
    {   859.865000,    0.1330,  7.989,   30.60,   0.68,  4.09,  0.84},
    {   899.407000,    0.0550,  7.917,   29.85,   0.68,  4.53,  0.90},
    {   902.555000,    0.0380,  8.432,   28.65,   0.70,  5.10,  0.95},
    {   906.205524,    0.1830,  5.111,   24.08,   0.70,  4.70,  0.53},
    {   916.171582,    8.5600,  1.442,   26.70,   0.70,  4.78,  0.78},
    {   970.315022,    9.1600,  1.920,   25.50,   0.64,  4.94,  0.67},
    {   987.926764,  138.0000,  0.258,   29.85,   0.68,  4.55,  0.90}};

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the MPM89 model 
  // (Liebe, Int. J. Infrared and Millimeter Waves, 10(6), 1989, 631):
  const Numeric CC_MPM89 = 1.00000;
  const Numeric CL_MPM89 = 1.00000;
  const Numeric CW_MPM89 = 1.00000;
  // ---------------------------------------------------------------------------------------


  // select the parameter set (!!model goes for values!!):
  Numeric CC, CL, CW;
  if ( model == "MPM89" )
    {
      CC = CC_MPM89;
      CL = CL_MPM89;
      CW = CW_MPM89;
    }
  else if ( model == "MPM89Lines" )
    {
      CC = 0.000;
      CL = CL_MPM89;
      CW = CW_MPM89;
    }
  else if ( model == "MPM89Continuum" )
    {
      CC = CC_MPM89;
      CL = 0.000;
      CW = 0.000;
    }
  else if ( model == "user" )
    {
      CC = CCin;
      CL = CLin;
      CW = CWin;
    }
  else
    {
      ostringstream os;
      os << "H2O-MPM89: ERROR! Wrong model values given.\n"
         << "Valid models are: 'MPM89', 'MPM89Lines', 'MPM89Continuum', and 'user'" << '\n';
      throw runtime_error(os.str());
    }
  out3  << "H2O-MPM89: (model=" << model << ") parameter values in use:\n" 
        << " CC = " << CC << "\n"
        << " CL = " << CL << "\n"
        << " CW = " << CW << "\n";
  
  
  // number of lines of Liebe line catalog (30 lines)
  const Index i_first = 0;
  const Index i_last  = 29;
  
  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );
  
  // Loop pressure/temperature (pressure in [hPa] therefore the factor 0.01)
  for ( Index i=0; i<n_p; ++i )
    {
      // here the total pressure is not multiplied by the H2O vmr for the 
      // P_H2O calculation because we calculate xsec and not abs: abs = vmr * xsec
      Numeric pwv_dummy = Pa_to_kPa * p_abs[i];
      // relative inverse temperature [1]
      Numeric theta     = (300.0 / t_abs[i]);
      // H2O partial pressure [kPa]
      Numeric pwv       = Pa_to_kPa * p_abs[i] * vmr[i];
      // dry air partial pressure [kPa]
      Numeric pda       = (Pa_to_kPa * p_abs[i]) - pwv;
      // H2O continuum absorption [dB/km/GHz^2] like in the original MPM89
      Numeric Nppc      = CC * pwv_dummy * pow(theta, (Numeric)3.0) * 1.000e-5
        * ( (0.113 * pda) + (3.57 * pwv * pow(theta, (Numeric)7.5)) );
      
      // Loop over input frequency
      for ( Index s=0; s<n_f; ++s )
        {
          // input frequency in [GHz]
          Numeric ff    = f_mono[s] * Hz_to_GHz; 
          // H2O line contribution at position f 
          Numeric Nppl  = 0.000;
          
          // Loop over MPM89 spectral lines:
          for ( Index l = i_first; l <= i_last; ++l )
            {
              // line strength [kHz]
              Numeric strength = CL * pwv_dummy * mpm89[l][1]
                * pow(theta, (Numeric)3.5) * exp(mpm89[l][2]*(1.000-theta));
              // line broadening parameter [GHz]
              Numeric gam      = CW * mpm89[l][3] * 0.001
                * ( mpm89[l][5] * pwv * pow(theta, mpm89[l][6]) +  
                                      pda * pow(theta, mpm89[l][4]) );
              // Doppler line width [GHz]
              // Numeric gamd     = 1.46e-6 * mpm89[l][0] / sqrt(theta);
              // effective line width [GHz]
              // gam              = 0.535 * gam + sqrt(0.217*gam*gam + gamd*gamd);  
              // H2O line absorption [dB/km/GHz] like in the original MPM89
              Nppl            += strength * MPMLineShapeFunction(gam, mpm89[l][0], ff); 
            }
          // xsec = abs/vmr [1/m] but MPM89 is in [dB/km] --> conversion necessary
          xsec(s,i) += dB_km_to_1_m * 0.1820 * ff * ( Nppl + (Nppc * ff) );
        }
    }
  return;
}
//
// #################################################################################
//
void MPM02H2OAbsModel( MatrixView        xsec,
                       const Numeric     CCin,       // continuum scale factor 
                       const Numeric     CLin,       // line strength scale factor
                       const Numeric     CWin,       // line broadening scale factor
                       const String&     model,
                       ConstVectorView   f_mono,
                       ConstVectorView   p_abs,
                       ConstVectorView   t_abs,
                       ConstVectorView   vmr )
{
  //
  /*
CTKS  OTHER DATA USED IF NOT FROM THEORETICAL CALC. IN A. BAUER ET AL. 41(1989)49-54:
CTKS  --------------------------------------------------------------------------------------------------------------
CTKS           | T=300 K       | T=300 K      |   T=300 K        |
CTKS  F     ISO|GWVHZO   NWVHZO| GWVNZ    NWVNZ|   GWVAIR   NWVAIR| REFERENCE
CTKS  GHZ   1  |MHZ/TORR 1     | MHZ/TORR 1    |   MHZ/TORR 1     |
CTKS  --------------------------------------------------------------------------------------------------------------
CTKS   22.2 1   18.00(18) -      4.10     --       3.77     --       LIEBE ET AL., J.CHEM.PHYS., 50(1969)727
CTKS  183.3 1   19.88    0.85    4.07(7)  0.63(10) 3.75(6)  0.64(10) A. BAUER ET AL. JQSRT 41(1989)49-54
CTKS  183.3 1    -        -      4.19(17) 0.74(3)  3.89(14) 0.76(3)  T. M. GOYETTE ET AL. J. MOLEC. SPEC, 143(1990)346
CTKS  203.4 2   --       --      4.214    0.93     3.833    0.89     J.-M. COLMONT ET AL. J. MOLEC. SPEC. 193(1999)233-243
CTKS  225.9 4   --       --      4.21     0.70     3.798    0.75     J.-M. COLMONT ET AL. J. MOLEC. SPEC. 193(1999)233-243
CTKS  241.6 4   --       --      4.45     0.77     4.08     0.80     J.-M. COLMONT ET AL. J. MOLEC. SPEC. 193(1999)233-243
CTKS  241.9 4   --       --      3.47     0.67     3.07     0.70     J.-M. COLMONT ET AL. J. MOLEC. SPEC. 193(1999)233-243
CTKS  325.1 1   --       --      4.011    0.63     3.633    0.64     J.-M. COLMONT ET AL. J. MOLEC. SPEC. 193(1999)233-243
CTKS  380.2 1   20.61(7) 0.89(1) 4.24(7)  0.52(14) 3.83(6)  0.54(14) A. BAUER ET AL. JQSRT 41(1987) 531
CTKS  380.2 1    -        -      4.16(4)  0.70(3)  3.80     0.72     T. M. GOYETTE ET AL. JQSRT 41(1993)485
CTKS  439.2 1   12.95(25)0.62(9)  --      --       --       --       V. N. MARKOV, J. MOLEC. SPEC, 164(1994)233
CTKS  752.0 1                    4.16(18) --       3.75     --       S. S. D. GASSTER ET AL. JOSA, 5(1988)593       
CTKS  987.9 1                    4.42(23) --       4.01     --       S. S. D. GASSTER ET AL. JOSA, 5(1988)593  
*/
  // Coefficients are from Liebe et al., AGARD CP-May93, Paper 3/1-10
  //         0             1        2       3        4       5      6
  //         f0            b1       b2      b3       b4      b5     b6
  //        [MHz]       [kHz/kPa]   [1]       [MHz/hPa]     [1]    [1]
  //                                        air      self   air    self
  const Numeric mpm02[35][7] = { 
    {    22235.0800,    0.10947,  2.1678,   2.811,   4.80,  0.69,  0.61},
    {    67803.9600,    0.00111,  8.7518,   2.858,   4.93,  0.69,  0.82},
    {   119995.9400,    0.00072,  8.3688,   2.948,   4.78,  0.70,  0.79},
    {   183310.1170,    2.30351,  0.6794,   3.050,   5.30,  0.76,  0.85},
    {   321225.6400,    0.04646,  6.1792,   2.303,   4.69,  0.67,  0.54},
    {   325152.9190,    1.53869,  1.5408,   2.783,   4.85,  0.68,  0.74},
    {   336227.6200,    0.00099,  9.8233,   2.693,   4.74,  0.64,  0.61},
    {   380197.3720,    11.9079,  1.0439,   2.873,   5.38,  0.72,  0.89},
    {   390134.5080,    0.00437,  7.3408,   2.152,   4.81,  0.63,  0.55},
    {   437346.6670,    0.06378,  5.0384,   1.845,   4.23,  0.60,  0.48},
    {   439150.8120,    0.92144,  3.5853,   2.100,   4.29,  0.63,  0.62},
    {   443018.2950,    0.19384,  5.0384,   1.860,   4.23,  0.60,  0.50},
    {   448001.0750,    10.6190,  1.3952,   2.632,   4.84,  0.66,  0.67},
    {   470888.9470,    0.33005,  3.5853,   2.152,   4.57,  0.66,  0.65},
    {   474689.1270,    1.27660,  2.3674,   2.355,   4.65,  0.65,  0.64},
    {   488491.1330,    0.25312,  2.8391,   2.602,   5.04,  0.69,  0.72},
    {   503568.5320,    0.03746,  6.7158,   1.612,   3.98,  0.61,  0.43},
    {   504482.6920,    0.01250,  6.7158,   1.612,   4.01,  0.61,  0.45},
    {   547676.4400,    1.01467,  0.1427,   2.600,   4.50,  0.69,  1.00}, // *
    {   552020.9600,    0.18668,  0.1452,   2.600,   4.50,  0.69,  1.00}, // *
    {   556936.0020,  510.51086,  0.1405,   3.210,   4.11,  0.69,  1.00},
    {   620700.8070,    5.10539,  2.3673,   2.438,   4.68,  0.71,  0.68},
    {   645905.6200,    0.00667,  8.6065,   1.800,   4.00,  0.60,  0.43},
    {   658006.5500,    0.27451,  7.7889,   3.210,   4.14,  0.69,  1.00},
    {   752033.2270,  249.68466,  0.3625,   3.060,   4.09,  0.68,  0.84},
    {   841051.1620,    0.01308,  8.1347,   1.590,   5.76,  0.33,  0.45},
    {   859965.6490,    0.13326,  8.0114,   3.060,   4.09,  0.68,  0.84},
    {   899302.1710,    0.05492,  7.8676,   2.985,   4.53,  0.68,  0.90},
    {   902609.4360,    0.03854,  8.3823,   2.865,   5.10,  0.70,  0.95},
    {   906206.1180,    0.18323,  5.0628,   2.408,   4.70,  0.70,  0.53},
    {   916171.5820,    8.56444,  1.3943,   2.670,   4.78,  0.70,  0.78},
    {   923113.1900,    0.00784, 10.2441,   2.900,   5.00,  0.66,  0.67},
    {   970315.0220,    9.16280,  1.8673,   2.550,   4.94,  0.64,  0.67},
    {   987926.7640,  138.28461,  0.2045,   2.985,   4.55,  0.68,  0.90},
  //--------------------------------------------------------------------
    {  1780.000000, 2230.00000,  0.952,  17.620,  30.50,  2.00,  5.00}}; // pseudo continuum line

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the MPM93 model (J. Liebe and G. A. Hufford and M. G. Cotton,
  // "Propagation modeling of moist air and suspended water/ice
  // particles at frequencies below 1000 GHz",
  // AGARD 52nd Specialists Meeting of the Electromagnetic Wave
  // Propagation Panel, Palma de Mallorca, Spain, 1993, May 17-21)
  const Numeric CC_MPM02 = 1.00000;
  const Numeric CL_MPM02 = 1.00000;
  const Numeric CW_MPM02 = 1.00000;
  // ---------------------------------------------------------------------------------------


  // select the parameter set (!!model dominates values!!):
  Numeric CC, CL, CW;
  // number of lines of Liebe line catalog (0-33 lines, 34 cont. pseudo line)
  Index i_first = 0;
  Index i_last  = 34;
  if ( model == "MPM02" )
    {
      CC      = CC_MPM02;
      CL      = CL_MPM02;
      CW      = CW_MPM02;
      i_first = 0;
      i_last  = 34;
    }
  else if ( model == "MPM02Lines" )
    {
      CC      = 0.000;
      CL      = CL_MPM02;
      CW      = CW_MPM02;
      i_first = 0;
      i_last  = 33;
    }
  else if ( model == "MPM02Continuum" )
    {
      CC      = CC_MPM02;
      CL      = 0.000;
      CW      = 0.000;
      i_first = 34;
      i_last  = 34;
    }
  else if ( model == "user" )
    {
      CC      = CCin;
      CL      = CLin;
      CW      = CWin;
      i_first = 0;
      i_last  = 34;

    }
  else
    {
      ostringstream os;
      os << "H2O-MPM02: ERROR! Wrong model values given.\n"
         << "Valid models are: 'MPM02', 'MPM02Lines', 'MPM02Continuum', and 'user'" << '\n';
      throw runtime_error(os.str());
    }
  out3  << "H2O-MPM02: (model=" << model << ") parameter values in use:\n" 
        << " CC = " << CC << "\n"
        << " CL = " << CL << "\n"
        << " CW = " << CW << "\n";
  
  
  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );

  // Loop pressure/temperature (pressure in hPa therefore the factor 0.01)
  for ( Index i=0; i<n_p; ++i )
    {
      // here the total pressure is not multiplied by the H2O vmr for the 
      // P_H2O calculation because we calculate xsec and not abs: abs = vmr * xsec
      Numeric pwv_dummy = Pa_to_hPa * p_abs[i];
      // relative inverse temperature [1]
      Numeric theta    = (300.0 / t_abs[i]);
      // H2O partial pressure [hPa]
      Numeric pwv      = Pa_to_hPa * p_abs[i] * vmr[i];
      // dry air partial pressure [hPa]
      Numeric pda      = (Pa_to_hPa * p_abs[i]) - pwv;
      // Loop over MPM02 spectral lines:
      
      // Loop over input frequency
      for ( Index s=0; s<n_f; ++s )
        {
          // input frequency in [GHz]
          Numeric ff = f_mono[s] * Hz_to_GHz; 
          
          for ( Index l = i_first; l <= i_last; ++l )
            {
              // line strength [ppm]. The missing vmr of H2O will be multiplied 
              // at the stage of absorption calculation: abs / vmr * xsec.
              Numeric strength = 0.00;
              Numeric gam = 0.00;
              if ( (l >= 0) && (l <= 33) ) // ---- just the lines ------------------
                {
                  strength = CL * pwv_dummy * mpm02[l][1] * 
                                  pow(theta, (Numeric)3.5)  * exp(mpm02[l][2]*(1.0-theta));
                  // line broadening parameter [GHz]
                  gam      = CW * mpm02[l][3] * 0.001 * 
                                  ( (mpm02[l][4] * pwv * pow(theta, mpm02[l][6])) +  
                                  (                pda * pow(theta, mpm02[l][5])) );
                }
              else if ( l == 34 ) // ----- just the continuum pseudo-line ----------
                {
                  strength = CC * pwv_dummy * mpm02[l][1] * 
                                  pow(theta, (Numeric)3.5)  * exp(mpm02[l][2]*(1.0-theta));
                  // line broadening parameter [GHz]
                  gam      = mpm02[l][3] * 0.001 * 
                             ( (mpm02[l][4] * pwv * pow(theta, mpm02[l][6])) +  
                             (                pda * pow(theta, mpm02[l][5])) );
                }
              else // ----- if something strange happens ---------------------------
                {
                  ostringstream os;
                  os << "H2O-MPM02: wrong line number detected l=" << l << " (0-34)\n";
                  throw runtime_error(os.str());
                  return;
                } // ---------------------------------------------------------------
              // Doppler line width [GHz]
              // Numeric gamd     = 1.46e-6 * mpm02[l][0] / sqrt(theta);
              // effective line width [GHz]
              //gam              = 0.535 * gam + sqrt(0.217*gam*gam + gamd*gamd); 
              // absorption [dB/km] like in the original MPM02
              Numeric Npp = strength * MPMLineShapeFunction(gam, mpm02[l][0], ff); 
              // xsec = abs/vmr [1/m] but MPM89 is in [dB/km] --> conversion necessary
              xsec(s,i)   += dB_km_to_1_m * 0.1820 * ff * Npp;
            }
        }
    }
  return;
}
//
//
// #################################################################################
//
void MPM93H2OAbsModel( MatrixView        xsec,
                       const Numeric     CCin,       // continuum scale factor 
                       const Numeric     CLin,       // line strength scale factor
                       const Numeric     CWin,       // line broadening scale factor
                       const String&     model,
                       ConstVectorView   f_mono,
                       ConstVectorView   p_abs,
                       ConstVectorView   t_abs,
                       ConstVectorView   vmr )
{
  //
  // Coefficients are from Liebe et al., AGARD CP-May93, Paper 3/1-10
  //         0           1        2       3        4      5      6
  //         f0          b1       b2      b3       b4     b5     b6
  //        [GHz]     [kHz/hPa]   [1]   [MHz/hPa]  [1]    [1]    [1]
  const Numeric mpm93[35][7] = { 
    {    22.235080,    0.01130,  2.143,   2.811,   4.80,  0.69,  1.00},
    {    67.803960,    0.00012,  8.735,   2.858,   4.93,  0.69,  0.82},
    {   119.995940,    0.00008,  8.356,   2.948,   4.78,  0.70,  0.79},
    {   183.310091,    0.24200,  0.668,   3.050,   5.30,  0.64,  0.85},
    {   321.225644,    0.00483,  6.181,   2.303,   4.69,  0.67,  0.54},
    {   325.152919,    0.14990,  1.540,   2.783,   4.85,  0.68,  0.74},
    {   336.222601,    0.00011,  9.829,   2.693,   4.74,  0.69,  0.61},
    {   380.197372,    1.15200,  1.048,   2.873,   5.38,  0.54,  0.89},
    {   390.134508,    0.00046,  7.350,   2.152,   4.81,  0.63,  0.55},
    {   437.346667,    0.00650,  5.050,   1.845,   4.23,  0.60,  0.48},
    {   439.150812,    0.09218,  3.596,   2.100,   4.29,  0.63,  0.52},
    {   443.018295,    0.01976,  5.050,   1.860,   4.23,  0.60,  0.50},
    {   448.001075,    1.03200,  1.405,   2.632,   4.84,  0.66,  0.67},
    {   470.888947,    0.03297,  3.599,   2.152,   4.57,  0.66,  0.65},
    {   474.689127,    0.12620,  2.381,   2.355,   4.65,  0.65,  0.64},
    {   488.491133,    0.02520,  2.853,   2.602,   5.04,  0.69,  0.72},
    {   503.568532,    0.00390,  6.733,   1.612,   3.98,  0.61,  0.43},
    {   504.482692,    0.00130,  6.733,   1.612,   4.01,  0.61,  0.45},
//    {   547.676440,    0.97010,  0.114,   2.600,   4.50,  0.70,  1.00},
//    {   552.020960,    1.47700,  0.114,   2.600,   4.50,  0.70,  1.00},
    {   547.676440,    0.97010*0.00199983,  0.114,   2.600,   4.50,  0.70,  1.00}, // isotopic ratio multiplied
    {   552.020960,    1.47700*0.00037200,  0.114,   2.600,   4.50,  0.70,  1.00}, // isotopic ratio multiplied
    {   556.936002,   48.74000,  0.159,   3.210,   4.11,  0.69,  1.00},
    {   620.700807,    0.50120,  2.200,   2.438,   4.68,  0.71,  0.68},
    {   645.866155,    0.00713,  8.580,   1.800,   4.00,  0.60,  0.50}, // ?? JPL tag 18003 (H2O) f_o = 645.7660100GHz
    {   658.005280,    0.03022,  7.820,   3.210,   4.14,  0.69,  1.00},
    {   752.033227,   23.96000,  0.396,   3.060,   4.09,  0.68,  0.84},
    {   841.053973,    0.00140,  8.180,   1.590,   5.76,  0.33,  0.45},
    {   859.962313,    0.01472,  7.989,   3.060,   4.09,  0.68,  0.84},
    {   899.306675,    0.00605,  7.917,   2.985,   4.53,  0.68,  0.90},
    {   902.616173,    0.00426,  8.432,   2.865,   5.10,  0.70,  0.95},
    {   906.207325,    0.01876,  5.111,   2.408,   4.70,  0.70,  0.53},
    {   916.171582,    0.83400,  1.442,   2.670,   4.78,  0.70,  0.78},
    {   923.118427,    0.00869, 10.220,   2.900,   5.00,  0.70,  0.80},
    {   970.315022,    0.89720,  1.920,   2.550,   4.94,  0.64,  0.67},
    {   987.926764,   13.21000,  0.258,   2.985,   4.55,  0.68,  0.90},
  //--------------------------------------------------------------------
    {  1780.000000, 2230.00000,  0.952,  17.620,  30.50,  2.00,  5.00}}; // pseudo continuum line

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the MPM93 model (J. Liebe and G. A. Hufford and M. G. Cotton,
  // "Propagation modeling of moist air and suspended water/ice
  // particles at frequencies below 1000 GHz",
  // AGARD 52nd Specialists Meeting of the Electromagnetic Wave
  // Propagation Panel, Palma de Mallorca, Spain, 1993, May 17-21)
  const Numeric CC_MPM93 = 1.00000;
  const Numeric CL_MPM93 = 1.00000;
  const Numeric CW_MPM93 = 1.00000;
  // ---------------------------------------------------------------------------------------


  // select the parameter set (!!model dominates values!!):
  Numeric CC, CL, CW;
  // number of lines of Liebe line catalog (0-33 lines, 34 cont. pseudo line)
  Index i_first = 0;
  Index i_last  = 34;
  if ( model == "MPM93" )
    {
      CC      = CC_MPM93;
      CL      = CL_MPM93;
      CW      = CW_MPM93;
      i_first = 0;
      i_last  = 34;
    }
  else if ( model == "MPM93Lines" )
    {
      CC      = 0.000;
      CL      = CL_MPM93;
      CW      = CW_MPM93;
      i_first = 0;
      i_last  = 33;
    }
  else if ( model == "MPM93Continuum" )
    {
      CC      = CC_MPM93;
      CL      = 0.000;
      CW      = 0.000;
      i_first = 34;
      i_last  = 34;
    }
  else if ( model == "user" )
    {
      CC      = CCin;
      CL      = CLin;
      CW      = CWin;
      i_first = 0;
      i_last  = 34;

    }
  else
    {
      ostringstream os;
      os << "H2O-MPM93: ERROR! Wrong model values given.\n"
         << "Valid models are: 'MPM93', 'MPM93Lines', 'MPM93Continuum', and 'user'" << '\n';
      throw runtime_error(os.str());
    }
  out3  << "H2O-MPM93: (model=" << model << ") parameter values in use:\n" 
        << " CC = " << CC << "\n"
        << " CL = " << CL << "\n"
        << " CW = " << CW << "\n";
  
  
  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );

  // Loop pressure/temperature (pressure in hPa therefore the factor 0.01)
  for ( Index i=0; i<n_p; ++i )
    {
      // here the total pressure is not multiplied by the H2O vmr for the 
      // P_H2O calculation because we calculate xsec and not abs: abs = vmr * xsec
      Numeric pwv_dummy = Pa_to_hPa * p_abs[i];
      // relative inverse temperature [1]
      Numeric theta    = (300.0 / t_abs[i]);
      // H2O partial pressure [hPa]
      Numeric pwv      = Pa_to_hPa * p_abs[i] * vmr[i];
      // dry air partial pressure [hPa]
      Numeric pda      = (Pa_to_hPa * p_abs[i]) - pwv;
      // Loop over MPM93 spectral lines:
      
      // Loop over input frequency
      for ( Index s=0; s<n_f; ++s )
        {
          // input frequency in [GHz]
          Numeric ff = f_mono[s] * Hz_to_GHz; 
          
          for ( Index l = i_first; l <= i_last; ++l )
            {
              // line strength [ppm]. The missing vmr of H2O will be multiplied 
              // at the stage of absorption calculation: abs / vmr * xsec.
              Numeric strength = 0.00;
              Numeric gam = 0.00;
              if ( (l >= 0) && (l <= 33) ) // ---- just the lines ------------------
                {
                  strength = CL * pwv_dummy * mpm93[l][1]
                    * pow(theta, (Numeric)3.5)  * exp(mpm93[l][2]*(1.0-theta));
                  // line broadening parameter [GHz]
                  gam      = CW * mpm93[l][3] * 0.001 * 
                                  ( (mpm93[l][4] * pwv * pow(theta, mpm93[l][6])) +  
                                  (                pda * pow(theta, mpm93[l][5])) );
                }
              else if ( l == 34 ) // ----- just the continuum pseudo-line ----------
                {
                  strength = CC * pwv_dummy * mpm93[l][1]
                    * pow(theta, (Numeric)3.5)  * exp(mpm93[l][2]*(1.0-theta));
                  // line broadening parameter [GHz]
                  gam      = mpm93[l][3] * 0.001 * 
                             ( (mpm93[l][4] * pwv * pow(theta, mpm93[l][6])) +  
                             (                pda * pow(theta, mpm93[l][5])) );
                }
              else // ----- if something strange happens ---------------------------
                {
                  ostringstream os;
                  os << "H2O-MPM93: wrong line number detected l=" << l << " (0-34)\n";
                  throw runtime_error(os.str());
                  return;
                } // ---------------------------------------------------------------
              // Doppler line width [GHz]
              // Numeric gamd     = 1.46e-6 * mpm93[l][0] / sqrt(theta);
              // effective line width [GHz]
              //gam              = 0.535 * gam + sqrt(0.217*gam*gam + gamd*gamd); 
              // absorption [dB/km] like in the original MPM93
              Numeric Npp = strength * MPMLineShapeFunction(gam, mpm93[l][0], ff); 
              // xsec = abs/vmr [1/m] but MPM89 is in [dB/km] --> conversion necessary
              xsec(s,i)   += dB_km_to_1_m * 0.1820 * ff * Npp;
            }
        }
    }
  return;
}
//
// #################################################################################
//
void PWR98H2OAbsModel( MatrixView        xsec,
                       const Numeric     CCin,       // continuum scale factor 
                       const Numeric     CLin,       // line strength scale factor
                       const Numeric     CWin,       // line broadening scale factor
                       const String&     model,
                       ConstVectorView   f_mono,
                       ConstVectorView   p_abs,
                       ConstVectorView   t_abs,
                       ConstVectorView   vmr )
{
  //   REFERENCES:
  //   LINE INTENSITIES FROM HITRAN92 (SELECTION THRESHOLD=
  //     HALF OF CONTINUUM ABSORPTION AT 1000 MB).
  //   WIDTHS MEASURED AT 22,183,380 GHZ, OTHERS CALCULATED:
  //     H.J.LIEBE AND T.A.DILLON, J.CHEM.PHYS. V.50, PP.727-732 (1969) &
  //     H.J.LIEBE ET AL., JQSRT V.9, PP. 31-47 (1969)  (22GHz);
  //     A.BAUER ET AL., JQSRT V.37, PP.531-539 (1987) & 
  //     ASA WORKSHOP (SEPT. 1989) (380GHz);
  //     AND A.BAUER ET AL., JQSRT V.41, PP.49-54 (1989) (OTHER LINES).
  //   AIR-BROADENED CONTINUUM BASED ON LIEBE & LAYTON, NTIA 
  //     REPORT 87-224 (1987); SELF-BROADENED CONTINUUM BASED ON 
  //     LIEBE ET AL, AGARD CONF. PROC. 542 (MAY 1993), 
  //     BUT READJUSTED FOR LINE SHAPE OF
  //     CLOUGH et al, ATMOS. RESEARCH V.23, PP.229-241 (1989).
  //
  // Coefficients are from P. W. Rosenkranz., Radio Science, 33(4), 919, 1998
  // line frequencies [GHz]
  const Numeric PWRfl[15] = {  22.2350800, 183.3101170, 321.2256400, 325.1529190, 380.1973720, 
                              439.1508120, 443.0182950, 448.0010750, 470.8889470,  474.6891270, 
                              488.4911330, 556.9360020,  620.7008070, 752.0332270, 916.1715820 };
  // line intensities at 300K [Hz * cm2] (see Janssen Appendix to Chap.2 for this)
  const Numeric PWRs1[15] = { 1.31e-14,  2.273e-12, 8.036e-14, 2.694e-12, 2.438e-11, 
                              2.179e-12, 4.624e-13, 2.562e-11, 8.369e-13, 3.263e-12, 
                              6.659e-13, 1.531e-9,  1.707e-11, 1.011e-9,  4.227e-11 };
  // T coeff. of intensities [1]
  const Numeric PWRb2[15] = { 2.144, 0.668, 6.179, 1.541, 1.048, 
                              3.595, 5.048, 1.405, 3.597, 2.379,
                              2.852, 0.159, 2.391, 0.396, 1.441 };
  // air-broadened width parameters at 300K [GHz/hPa]
  const Numeric PWRw3[15] = { 0.00281, 0.00281, 0.00230, 0.00278, 0.00287,
                              0.00210, 0.00186, 0.00263, 0.00215, 0.00236,
                              0.00260, 0.00321, 0.00244, 0.00306, 0.00267 };
  // T-exponent of air-broadening [1]
  const Numeric PWRx[15]  = { 0.69, 0.64, 0.67, 0.68, 0.54,
                              0.63, 0.60, 0.66, 0.66, 0.65,
                              0.69, 0.69, 0.71, 0.68, 0.70 };
  // self-broadened width parameters at 300K [GHz/hPa]
  const Numeric PWRws[15] = { 0.01349, 0.01491, 0.01080, 0.01350, 0.01541,
                              0.00900, 0.00788, 0.01275, 0.00983, 0.01095,
                              0.01313, 0.01320, 0.01140, 0.01253, 0.01275 };

  // T-exponent of self-broadening [1]
  const Numeric PWRxs[15] = { 0.61, 0.85, 0.54, 0.74, 0.89,
                              0.52, 0.50, 0.67, 0.65, 0.64,
                              0.72, 1.00, 0.68, 0.84, 0.78 };
 
   // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the MPM87 model (P. W. Rosenkranz., Radio Science, 33(4), 919, 1998):
  const Numeric CC_PWR98 = 1.00000;
  const Numeric CL_PWR98 = 1.00000;
  const Numeric CW_PWR98 = 1.00000;
  // ---------------------------------------------------------------------------------------


  // select the parameter set (!!model dominates values!!):
  Numeric CC, CL, CW;
  if ( model == "Rosenkranz" )
    {
      CC = CC_PWR98;
      CL = CL_PWR98;
      CW = CW_PWR98;
    }
  else if ( model == "RosenkranzLines" )
    {
      CC = 0.000;
      CL = CL_PWR98;
      CW = CW_PWR98;
    }
  else if ( model == "RosenkranzContinuum" )
    {
      CC = CC_PWR98;
      CL = 0.000;
      CW = 0.000;
    }
  else if ( model == "user" )
    {
      CC = CCin;
      CL = CLin;
      CW = CWin;
    }
  else
    {
      ostringstream os;
      os << "H2O-PWR98: ERROR! Wrong model values given.\n"
         << "Valid models are: 'Rosenkranz', 'RosenkranzLines', 'RosenkranzContinuum', and 'user'" << '\n';
      throw runtime_error(os.str());
    }
  out3  << "H2O-PWR98: (model=" << model << ") parameter values in use:\n" 
        << " CC = " << CC << "\n"
        << " CL = " << CL << "\n"
        << " CW = " << CW << "\n";
  
  
  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );

  // Loop pressure/temperature:
  for ( Index i=0; i<n_p; ++i )
    {
      // here the total pressure is not multiplied by the H2O vmr for the 
      // P_H2O calculation because we calculate xsec and not abs: abs = vmr * xsec
      Numeric pvap_dummy = Pa_to_hPa * p_abs[i];
      // water vapor partial pressure [hPa]
      Numeric pvap       = Pa_to_hPa * p_abs[i] * vmr[i];
      // dry air partial pressure [hPa]
      Numeric pda        = (Pa_to_hPa * p_abs[i]) - pvap;
      // Rosenkranz number density  (Rosenkranz H2O mass density in [g/m³])
      // [g/m³]    =  [g*K / Pa*m³]  *  [Pa/K]
      // rho       =   (M_H2O / R)   *  (P_H2O / T)
      // rho       =      2.1667     *  p_abs * vmr / t_abs
      // den       = 3.335e16 * rho
      // FIXME Numeric den        = 3.335e16 * (2.1667 * p_abs[i] * vmr[i] / t_abs[i]);
      Numeric den_dummy  = 3.335e16 * (2.1667 * p_abs[i] / t_abs[i]);
      // inverse relative temperature [1]
      Numeric ti         = (300.0 / t_abs[i]);
      Numeric ti2        = pow(ti, (Numeric)2.5);
      
      // continuum term [Np/km/GHz2]
      Numeric con = CC * pvap_dummy * pow(ti, (Numeric)3.0) * 1.000e-9
        * ( (0.543 * pda) + (17.96 * pvap * pow(ti, (Numeric)4.5)) );
          
      // Loop over input frequency
      for ( Index s=0; s<n_f; ++s )
        {
          // input frequency in [GHz]
          Numeric ff  = f_mono[s] * Hz_to_GHz;
          // line contribution at position f
          Numeric sum = 0.000;
          
          // Loop over spectral lines
          for (Index l = 0; l < 15; l++) 
            {
              Numeric width    = ( CW * PWRw3[l] * pda  * pow(ti, PWRx[l]) ) + 
                                 (      PWRws[l] * pvap * pow(ti, PWRxs[l]));
              //              Numeric width    = CW * ( PWRw3[l] * pda  * pow(ti, PWRx[l]) + 
              //                                        PWRws[l] * pvap * pow(ti, PWRxs[l]) );
              Numeric wsq      = width * width;
              Numeric strength = CL * PWRs1[l] * ti2 * exp(PWRb2[l]*(1.0 - ti));
              // frequency differences
              Numeric df0      = ff - PWRfl[l];
              Numeric df1      = ff + PWRfl[l];
              // use Clough's definition of local line contribution
              Numeric base     = width / (wsq + 562500.000);
              // positive and negative resonances
              Numeric res      = 0.000;
              if (fabs(df0) < 750.0) res += width / (df0*df0 + wsq) - base;
              if (fabs(df1) < 750.0) res += width / (df1*df1 + wsq) - base;
              sum             += strength * res * pow( (ff/PWRfl[l]),
                                                       (Numeric)2.0 );
            }
          // line term [Np/km]
          Numeric absl = 0.3183e-4 * den_dummy * sum;
          // xsec = abs/vmr [1/m] (Rosenkranz model in [Np/km])
          // 4.1907e-5 = 0.230259 * 0.1820 * 1.0e-3    (1/(10*log(e)) = 0.230259)
          xsec(s,i)  += 1.000e-3 * ( absl + (con * ff * ff) );    
        }
    }
  return;
}
//
// #################################################################################
//
void CP98H2OAbsModel( MatrixView        xsec,
                      const Numeric     CCin,       // continuum scale factor 
                      const Numeric     CLin,       // line strength scale factor
                      const Numeric     CWin,       // line broadening scale factor
                      const String&     model,
                      ConstVectorView   f_mono,
                      ConstVectorView   p_abs,
                      ConstVectorView   t_abs,
                      ConstVectorView   vmr )
{

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the CP98 model (S. L. Cruz-Pol et al., Radio Science, 33(5), 1319, 1998):
  const Numeric CC_CP98 = 1.2369; // +/- 0.155  !LARGE!
  const Numeric CL_CP98 = 1.0639; // +/- 0.016
  const Numeric CW_CP98 = 1.0658; // +/- 0.0096
  // ---------------------------------------------------------------------------------------

  // select the parameter set (!!model dominates values!!):
  Numeric CC, CL, CW;
  if ( model == "CruzPol" )
    {
      CC = CC_CP98;
      CL = CL_CP98;
      CW = CW_CP98;
    }
  else if ( model == "CruzPolLine" )
    {
      CC = 0.000;
      CL = CL_CP98;
      CW = CW_CP98;
    }
  else if ( model == "CruzPolContinuum" )
    {
      CC = CC_CP98;
      CL = 0.000;
      CW = 0.000;
    }
  else if ( model == "user" )
    {
      CC = CCin;
      CL = CLin;
      CW = CWin;
    }
  else
    {
      ostringstream os;
      os << "H2O-CP98: ERROR! Wrong model values given.\n"
         << "Valid models are: 'CruzPol', 'CruzPolLine', 'CruzPolContinuum', and 'user'" << "\n";
      throw runtime_error(os.str());
    }
  out3  << "H2O-CP98: (model=" << model << ") parameter values in use:\n" 
        << " CC = " << CC << "\n"
        << " CL = " << CL << "\n"
        << " CW = " << CW << "\n";
  
  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );

  // Loop pressure/temperature (pressure in [hPa] therefore the factor 0.01)
  for ( Index i=0; i<n_p; ++i )
    {
      // calculate xsec only if VMR(H2O) > VMRCalcLimit
      if (vmr[i] > VMRCalcLimit)
        {
          // relative inverse temperature [1]
          Numeric theta = (300.0 / t_abs[i]);
          // H2O partial pressure [hPa]
          Numeric pwv   = Pa_to_hPa * p_abs[i] * vmr[i];
          // dry air partial pressure [hPa]
          Numeric pda   = (Pa_to_hPa * p_abs[i]) - pwv;
          // line strength
          Numeric TL    = CL * 0.0109 * pwv * pow(theta,(Numeric)3.5)
            * exp(2.143*(1.0-theta));
          // line broadening parameter [GHz]
          Numeric gam   = CW * 0.002784 *  
                          ( (pda * pow(theta,(Numeric)0.6))
                            + (4.80 * pwv * pow(theta,(Numeric)1.1)) );
          // continuum term
          Numeric TC    = CC * pwv * pow(theta, (Numeric)3.0) * 1.000e-7
            * ( (0.113 * pda) + (3.57 * pwv * pow(theta,(Numeric)7.5)) );

          // Loop over input frequency
          for ( Index s=0; s<n_f; ++s )
            {
              // input frequency in [GHz]
              Numeric ff  = f_mono[s] * Hz_to_GHz; 
              Numeric TSf = MPMLineShapeFunction(gam, 22.235080, ff); 
              // xsec = abs/vmr [1/m] (Cruz-Pol model in [Np/km])
              xsec(s,i) += 4.1907e-5 * ff * ( (TL * TSf) + (ff * TC) ) / vmr[i];
            }
        }
    }
  return;
}
//
// #################################################################################
//
void Standard_H2O_self_continuum( MatrixView        xsec,
                                  const Numeric     Cin,
                                  const Numeric     xin,
                                  const String&     model,
                                  ConstVectorView   f_mono,
                                  ConstVectorView   p_abs,
                                  ConstVectorView   t_abs,
                                  ConstVectorView   vmr  )
{

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the Rosenkranz model (Radio Science, 33(4), 919, 1998):
  const Numeric Cs_PWR   = 1.796e-33;  //  [1/m / (Hz²*Pa²)]
  const Numeric xs_PWR   = 4.5;        //  [1]
  // standard values for the Cruz-Pol model (Radio Science, 33(5), 1319, 1998):
  const Numeric Cs_CP    = 1.851e-33;  //  [1/m / (Hz²*Pa²)]
  const Numeric xs_CP    = 7.5;        //  [1]
  // standard values for the MPM89 model (Int. J. Inf. and Millim. Waves, 10(6), 1989, 631):
  const Numeric Cs_MPM89 = 1.500e-33;  //  [1/m / (Hz²*Pa²)]
  const Numeric xs_MPM89 = 7.5;        //  [1]
  // standard values for the MPM87 model (Radio Science, 20(5), 1985, 1069):
  const Numeric Cs_MPM87 = 1.500e-33;  //  [1/m / (Hz²*Pa²)]
  const Numeric xs_MPM87 = 7.5;        //  [1]
  // ---------------------------------------------------------------------------------------

  // select the parameter set (!!model goes for values!!):
  Numeric C, x;
   if ( model == "Rosenkranz" )
     {
       C = Cs_PWR;
       x = xs_PWR;
     }
   else if ( model == "CruzPol" )
     {
       C = Cs_CP;
       x = xs_CP;
     }
   else if ( model == "MPM89" )
     {
       C = Cs_MPM89;
       x = xs_MPM89;
     }
   else if ( model == "MPM87" )
     {
       C = Cs_MPM87;
       x = xs_MPM87;
     }
   else if ( model == "user" )
     {
       C = Cin;
       x = xin;
     }
   else
     {
       ostringstream os;
       os << "H2O-SelfContStandardType: ERROR! Wrong model values given.\n"
          << "allowed models are: 'Rosenkranz', 'CruzPol', 'MPM89', 'MPM87', 'user'" << '\n';
       throw runtime_error(os.str());
     }
   out3  << "H2O-SelfContStandardType: (model=" << model << ") parameter values in use:\n" 
         << " C_s = " << C << "\n"
         << " x_s = " << x << "\n";



  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );
  
  // Loop over pressure/temperature grid:
  for ( Index i=0; i<n_p; ++i )
    {
      // Dummy scalar holds everything except the quadratic frequency dependence.
      // The second vmr of H2O will be multiplied at the stage of absorption 
      // calculation: abs = vmr * xsec.
      Numeric dummy =
        C * pow( (Numeric)300./t_abs[i], x+(Numeric)3. )
        * pow( p_abs[i], (Numeric)2. ) * vmr[i];

      // Loop over frequency grid:
      for ( Index s=0; s<n_f; ++s )
        {
          xsec(s,i) += dummy * pow( f_mono[s], (Numeric)2. );
          //      cout << "xsec(" << s << "," << i << "): " << xsec(s,i) << "\n";
        }
    }
}
//
// #################################################################################
//
void Standard_H2O_foreign_continuum( MatrixView        xsec,
                                     const Numeric     Cin,
                                     const Numeric     xin,
                                     const String&     model,
                                     ConstVectorView   f_mono,
                                     ConstVectorView   p_abs,
                                     ConstVectorView   t_abs,
                                     ConstVectorView   vmr       )
{

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the Rosenkranz model (Radio Science, 33(4), 919, 1998):
  const Numeric Cf_PWR   = 5.43e-35 ;  //  [1/m / (Hz²*Pa²)]
  const Numeric xf_PWR   = 0.0;        //  [1]
  // standard values for the Cruz-Pol model (Radio Science, 33(5), 1319, 1998):
  const Numeric Cf_CP    = 5.85e-35;  //  [1/m / (Hz²*Pa²)]
  const Numeric xf_CP    = 0.0;        //  [1]
  // standard values for the MPM89 model (Int. J. Inf. and Millim. Waves, 10(6), 1989, 631):
  const Numeric Cf_MPM89 = 4.74e-35;  //  [1/m / (Hz²*Pa²)]
  const Numeric xf_MPM89 = 0.0;        //  [1]
  // standard values for the MPM87 model (Radio Science, 20(5), 1985, 1069):
  const Numeric Cf_MPM87 = 4.74e-35;  //  [1/m / (Hz²*Pa²)]
  const Numeric xf_MPM87 = 0.0;        //  [1]
  // ---------------------------------------------------------------------------------------


  // select the parameter set (!!model goes for values!!):
  Numeric C, x;
   if ( model == "Rosenkranz" )
     {
       C = Cf_PWR;
       x = xf_PWR;
     }
   else if ( model == "CruzPol" )
     {
       C = Cf_CP;
       x = xf_CP;
     }
   else if ( model == "MPM89" )
     {
       C = Cf_MPM89;
       x = xf_MPM89;
     }
   else if ( model == "MPM87" )
     {
       C = Cf_MPM87;
       x = xf_MPM87;
     }
   else if ( model == "user" )
     {
       C = Cin;
       x = xin;
     }
   else
     {
       ostringstream os;
       os << "H2O-ForeignContStandardType: ERROR! Wrong model values given.\n"
          << "allowed models are: 'Rosenkranz', 'CruzPol', 'MPM89', 'MPM87', 'user'" << '\n';
       throw runtime_error(os.str());
     }
   out3  << "H2O-ForeignContStandardType: (model=" << model << ") parameter values in use:\n" 
         << " C_s = " << C << "\n"
         << " x_s = " << x << "\n";

  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );
  
  // Loop pressure/temperature:
  for ( Index i=0; i<n_p; ++i )
    {
      // Dry air partial pressure: p_dry := p_tot - p_h2o.
      Numeric pdry  = p_abs[i] * (1.000e0-vmr[i]);
      // Dummy scalar holds everything except the quadratic frequency dependence.
      // The vmr of H2O will be multiplied at the stage of absorption 
      // calculation: abs = vmr * xsec.
      Numeric dummy = C * pow( (Numeric)300./t_abs[i], x+(Numeric)3. )
        * p_abs[i] * pdry;

      // Loop frequency:
      for ( Index s=0; s<n_f; ++s )
        {
          xsec(s,i) += dummy * pow( f_mono[s], (Numeric)2. );
          //      cout << "xsec(" << s << "," << i << "): " << xsec(s,i) << "\n";
        }
    }
}
//
//
// #################################################################################
//
void MaTipping_H2O_foreign_continuum( MatrixView        xsec,
                                      const Numeric      Cin,
                                      const Numeric      xin,
                                      const String&     model,
                                      ConstVectorView   f_mono,
                                      ConstVectorView   p_abs,
                                      ConstVectorView   t_abs,
                                      ConstVectorView   vmr      )
{

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for Q. Ma and R. H. Tipping, J. Chem. Phys., 117(23), 10581, 2002:
  // the Cf value is originally given in dB/km/kPa^2/GHz^2.0389. the conversion factor is 
  // then 1.0283E-28 to get arts units. Additionally the Cf value is divided by 1.08 to 
  // get the Cf for air.
  const Numeric Cf_MaTipping = 1.8590e-35;   //  [1/m / (Hz²*Pa²)]
  const Numeric xf_MaTipping = 4.6019;       //  [1]
  // ---------------------------------------------------------------------------------------


  // select the parameter set (!!model goes for values!!):
  Numeric C, x;
   if ( model == "MaTipping" )
     {
       C = Cf_MaTipping;
       x = xf_MaTipping;
     }
   else if ( model == "user" )
     {
       C = Cin;
       x = xin;
     }
   else
     {
       ostringstream os;
       os << "H2O-MaTipping_H2O_foreign_continuum: ERROR! Wrong model values given.\n"
          << "allowed models are: 'MaTipping', 'user'" << '\n';
       throw runtime_error(os.str());
     }
   out3  << "H2O-MaTipping_H2O_foreign_continuum: (model=" << model << ") parameter values in use:\n" 
         << " C_s = " << C << "\n"
         << " x_s = " << x << "\n";

  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );
  
  // Loop pressure/temperature:
  for ( Index i=0; i<n_p; ++i )
    {
      // Dry air partial pressure: p_dry := p_tot - p_h2o.
      Numeric pdry  = p_abs[i] * (1.000e0-vmr[i]);
      // Dummy scalar holds everything except the quadratic frequency dependence.
      // The vmr of H2O will be multiplied at the stage of absorption 
      // calculation: abs = vmr * xsec.
      Numeric dummy = C * pow( (Numeric)300./t_abs[i], x )
        * p_abs[i] * pdry;

      // Loop frequency:
      for ( Index s=0; s<n_f; ++s )
        {
          xsec(s,i) += dummy * pow( f_mono[s], (Numeric)2.0389 );
          //      cout << "xsec(" << s << "," << i << "): " << xsec(s,i) << "\n";
        }
    }
}
//
// #################################################################################



// =================================================================================


Numeric XINT_FUN( const Numeric V1A,
                  const Numeric /* V2A */,
                  const Numeric DVA,
                  const Numeric A[],
                  const Numeric VI)
{

// ----------------------------------------------------------------------
  //     THIS SUBROUTINE INTERPOLATES THE A ARRAY STORED               
  //     FROM V1A TO V2A IN INCREMENTS OF DVA INTO XINT
// ----------------------------------------------------------------------

  const Numeric ONEPL  = 1.001;     // original value given in F77 code
  // FIXME const Numeric ONEMI  = 0.999;     // original value given in F77 code

  //const Numeric ONEPL  = 0.001;  // modified value for C/C++ code

  Numeric RECDVA = 1.00e0/DVA;
    
  int J      = (int) ((VI-V1A)*RECDVA + ONEPL) ; 
  Numeric VJ = V1A + DVA * (Numeric)(J-1);    
  Numeric P  = RECDVA * (VI-VJ);        
  Numeric C  = (3.00e0-2.00e0*P) * P * P;         
  Numeric B  = 0.500e0 * P * (1.00e0-P);          
  Numeric B1 = B * (1.00e0-P);              
  Numeric B2 = B * P;                   
  
  Numeric xint = -A[J-1] * B1             +
                  A[J]   * (1.00e0-C+B2)  + 
                  A[J+1] * (C+B1)         - 
                  A[J+2] * B2;

  /*
  cout << (J-1) << " <-> " << (J+2)  
       << ",  V=" << VI << ", VJ=" << VJ << "\n";
  cout << "xint=" << xint  << " " << A[J-1] << " " << A[J] << " " << A[J+1] << " " << A[J+2] << "\n";
  */

  return xint;
}

// =================================================================================

Numeric RADFN_FUN (const Numeric VI, 
                   const Numeric XKT)
{
// ---------------------------------------------------------------------- B18060
//              LAST MODIFICATION:    12 AUGUST 1991                      B17940
//                                                                        B17950
//                 IMPLEMENTATION:    R.D. WORSHAM                        B17960
//                                                                        B17970
//            ALGORITHM REVISIONS:    S.A. CLOUGH                         B17980
//                                    R.D. WORSHAM                        B17990
//                                    J.L. MONCET                         B18000
//                                                                        B18010
//                                                                        B18020
//                    ATMOSPHERIC AND ENVIRONMENTAL RESEARCH INC.         B18030
//                    840 MEMORIAL DRIVE,  CAMBRIDGE, MA   02139          B18040
//                                                                        B18050
//                                                                        B18070
//              WORK SUPPORTED BY:    THE ARM PROGRAM                     B18080
//                                    OFFICE OF ENERGY RESEARCH           B18090
//                                    DEPARTMENT OF ENERGY                B18100
//                                                                        B18110
//                                                                        B18120
//     SOURCE OF ORIGINAL ROUTINE:    AFGL LINE-BY-LINE MODEL             B18130
//                                                                        B18140
//                                            FASCOD3                     B18150
//                                                                        B18160
// ---------------------------------------------------------------------- B18060
//                                                                        B18170
//  IN THE SMALL XVIOKT REGION 0.5 IS REQUIRED

  Numeric XVI   = VI;                            
  Numeric RADFN = 0.00e0;                                
                                                                           
  if (XKT > 0.0)
    {                                    
      Numeric XVIOKT = XVI/XKT;                 
      
      if (XVIOKT <= 0.01e0)
        {
          RADFN = 0.500e0 * XVIOKT * XVI;
        }
      else if (XVIOKT <= 10.0e0)
        {
          Numeric EXPVKT = exp(-XVIOKT);
          RADFN = XVI * (1.00e0-EXPVKT) / (1.00e0+EXPVKT);
        }
      else
        {
          RADFN = XVI;                         
        }                                  
    }
  else
    {
      RADFN = XVI;
    }
  
  return RADFN;
}

// =================================================================================

// CKD version 2.2.2 H2O self continuum absorption model
void CKD_222_self_h2o( MatrixView          xsec,
                       const Numeric       Cin,
                       const String&       model,
                       ConstVectorView     f_mono,
                       ConstVectorView     p_abs,
                       ConstVectorView     t_abs,
                       ConstVectorView     vmr,
                       ConstVectorView     /* n2_abs */ )
{


  // check the model name about consistency
  if ((model != "user") &&  (model != "CKD222"))
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKDv2.2.2 H2O self continuum:\n"
         << "INPUT model name is: " << model << ".\n"
         << "VALID model names are user and CKD222\n";
      throw runtime_error(os.str());
    }


  // scaling factor of the self H2O cont. absorption
  Numeric  ScalingFac = 1.0000e0;
  if ( model == "user" )
    {
      ScalingFac = Cin; // input scaling factor of calculated absorption
    }


  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies


  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );


  // ************************** CKD stuff ************************************

  const Numeric xLosmt   = 2.686763e19; // [molecules/cm^3]
  // FIXME const Numeric T1       =  273.0e0;
  const Numeric TO       =  296.0e0;
  const Numeric PO       = 1013.0e0;

  // CKD2.2.2 specific self continuum correction function parameters
  const Numeric ALPHA2 = 200.000 * 200.000;
  const Numeric ALPHS2 = 120.000 * 120.000;
  const Numeric BETAS  = 5.000e-06;
  const Numeric V0S    = 1310.000;
  const Numeric FACTRS = 0.150;
  
  // These are self-continuum modification factors from 700-1200 cm-1
  const Numeric XFAC[51] = {  
    1.00000,1.01792,1.03767,1.05749,1.07730,1.09708,
    1.10489,1.11268,1.12047,1.12822,1.13597,1.14367,
    1.15135,1.15904,1.16669,1.17431,1.18786,1.20134,
    1.21479,1.22821,1.24158,1.26580,1.28991,1.28295,
    1.27600,1.26896,1.25550,1.24213,1.22879,1.21560,
    1.20230,1.18162,1.16112,1.14063,1.12016,1.10195,
    1.09207,1.08622,1.08105,1.07765,1.07398,1.06620,
    1.05791,1.04905,1.03976,1.02981,1.00985,1.00000,
    1.00000,1.00000,1.00000};

  // wavenumber range where CKD H2O self continuum is valid
  const Numeric VABS_min = SL260_ckd_0_v1; // [cm^-1]
  const Numeric VABS_max = SL260_ckd_0_v2; // [cm^-1]


  // It is assumed here that f_mono is monotonically increasing with index!
  // In future change this return into a change of the loop over
  // the frequency f_mono. n_f_new < n_f
  Numeric V1ABS = f_mono[0]     / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  Numeric V2ABS = f_mono[n_f-1] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  if ( (V1ABS < VABS_min) || (V1ABS > VABS_max) ||
       (V2ABS < VABS_min) || (V2ABS > VABS_max) )
    {
      out3  << "WARNING:\n"
            << "  CKD2.2.2 H2O self continuum:\n"
            << "  input frequency vector exceeds range of model validity\n"
            << "  " << SL296_ckd_0_v1 << "<->" << SL296_ckd_0_v2 << "cm^-1\n";
    }


  // ------------------- subroutine SL296/SL260 ----------------------------

  if (SL296_ckd_0_v1 != SL260_ckd_0_v1)
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD2.2.2 H2O self continuum:\n"
         << "parameter V1 not the same for different ref. temperatures.\n";
      throw runtime_error(os.str());
    }
  if (SL296_ckd_0_v2 != SL260_ckd_0_v2)
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD2.2.2 H2O self continuum:\n"
         << "parameter V2 not the same for different ref. temperatures.\n";
        throw runtime_error(os.str());
    }
  if (SL296_ckd_0_dv != SL260_ckd_0_dv)
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD2.2.2 H2O self continuum:\n"
         << "parameter DV not the same for different ref. temperatures.\n";
      throw runtime_error(os.str());
    }
  if (SL296_ckd_0_npt != SL260_ckd_0_npt)
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD2.2.2 H2O self continuum:\n"
         << "parameter NPT not the same for different ref. temperatures.\n";
      throw runtime_error(os.str());
    }
  
  // retrieve the appropriate array sequence of the self continuum
  // arrays of the CKD model.
  Numeric DVC = SL296_ckd_0_dv;
  Numeric V1C = V1ABS - DVC;
  Numeric V2C = V2ABS + DVC;
  
  int I1 = (int) ((V1C-SL296_ckd_0_v1) / SL296_ckd_0_dv);
  if (V1C < SL296_ckd_0_v1) I1 = -1;
  V1C = SL296_ckd_0_v1 + (SL296_ckd_0_dv * (Numeric)I1);

  int I2 = (int) ((V2C-SL296_ckd_0_v1) / SL296_ckd_0_dv);

  int NPTC = I2-I1+3;
  if (NPTC > SL296_ckd_0_npt) NPTC = SL296_ckd_0_npt+1;

  V2C = V1C + SL296_ckd_0_dv * (Numeric)(NPTC-1);  
  
  if (NPTC < 1)
    {
      ostringstream os;
      out3 << "WARNING:\n"  
           << "  CKD2.2.2 H2O self continuum:\n"
           << "  no elements of internal continuum coefficients could be found for the\n"
           << "  input frequency range.\n"
           << "  Leave the function without calculating the absorption.";
      return;
    }

  Numeric SH2OT0[NPTC+addF77fields]; // [cm^3/molecules]
  Numeric SH2OT1[NPTC+addF77fields]; // [cm^3/molecules]

  for (Index J = 1 ; J <= NPTC ; ++J)
    {
      Index I = I1+J;
      if ( (I < 1) || (I > SL296_ckd_0_npt) ) 
        {
          SH2OT0[J] = 0.0e0;   // at T=296 K
          SH2OT1[J] = 0.0e0;   // at T=260 K
        }
      else
        {
          SH2OT0[J] = SL296_ckd_0[I];    // at T=296 K
          SH2OT1[J] = SL260_ckd_0[I];    // at T=260 K 
        }
    }

  // ------------------- subroutine SL296/SL260 ----------------------------
  
  Numeric SFAC = 1.00e0;
  Numeric VS2  = 0.00e0;
  // FIXME Numeric VS4  = 0.00e0;
  
  // Loop pressure/temperature:
  for ( Index i = 0 ; i < n_p ; ++i )
    {

      // atmospheric state parameters
      Numeric Tave   = t_abs[i];                                     // [K]
      Numeric Pave   = (p_abs[i]*1.000e-2);                          // [hPa]
      Numeric Patm   = Pave/PO;                                      // [1]
      Numeric vmrh2o = vmr[i];                                       // [1]
      // FIXME Numeric Ph2o   = Patm * vmrh2o;                                // [1]
      // second vmr in absCalc multiplied
      Numeric Rh2o   = Patm * (TO/Tave);                             // [1]
      Numeric Tfac   = (Tave-TO)/(260.0-TO);                         // [1]
      Numeric WTOT   = xLosmt * (Pave/1.013000e3) * (2.7300e2/Tave); // [molecules/cm^2]
      Numeric W1     = vmrh2o * WTOT;                                // [molecules/cm^2]
      Numeric XKT    = Tave / 1.4387752e0;                           // = (T*k_B)/(h*c)    
      
      // Molecular cross section calculated by CKD.
      // The cross sectionis calculated on the predefined 
      // CKD wavenumber grid.
      Numeric k[NPTC+addF77fields]; // [1/cm]
      k[0] = 0.00e0; // not used array field
      for (Index J = 1 ; J <= NPTC ; ++J)
        {
          Numeric VJ   = V1C + (DVC * (Numeric)(J-1)); 
          Numeric SH2O = 0.0e0;
          if (SH2OT0[J] > 0.0e0)
            {
              SH2O = SH2OT0[J] * pow( (SH2OT1[J]/SH2OT0[J]), Tfac ); 
              SFAC = 1.00e0;

              if ( (VJ >= 700.0e0) && (VJ <= 1200.0e0) )
                {
                  int JFAC = (int)((VJ - 700.0e0)/10.0e0 + 0.00001e0);
                  if ( (JFAC >= 0) && (JFAC <= 50) )
                    SFAC = XFAC[JFAC];
                }

              // ---------------------------------------------------------
              // Correction to self continuum (1 SEPT 85); factor of    
              // 0.78 at 1000 and  .......

              VS2  = (VJ-V0S) * (VJ-V0S);

              SFAC = SFAC * 
                ( 1.000e0 + 0.3000e0 * (1.000e4 / ((VJ*VJ)                         + 1.000e4))  ) *   
                ( 1.000e0 - 0.2333e0 * (ALPHA2  / ((VJ-1050.000e0)*(VJ-1050.000e0) + ALPHA2))   ) *   
                ( 1.000e0 - FACTRS   * (ALPHS2  / (VS2+(BETAS*VS2*VS2)+ALPHS2))                 );

              SH2O = SFAC * SH2O;
            }

          // CKD cross section with radiative field [1/cm]
          // the VMRH2O will be multiplied in absCalc, hence Rh2o does not contain 
          // VMRH2O as multiplicative term
          k[J] = W1 * Rh2o * (SH2O*1.000e-20) * RADFN_FUN(VJ,XKT); // [1]

        }
      

      // Loop input frequency array. The previously calculated cross section 
      // has therefore to be interpolated on the input frequencies.
      for ( Index s = 0 ; s < n_f ; ++s )
        {
          // calculate the associated wave number (= 1/wavelength)
          Numeric V = f_mono[s] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
          if ( (V >= 0.000e0) && (V < SL296_ckd_0_v2) )
            {
              // arts cross section [1/m]
              // interpolate the k vector on the f_mono grid
              // The factor 100 comes from the conversion from 1/cm to 1/m for
              // the absorption coefficient
              xsec(s,i) +=  ScalingFac * 1.000e2 * XINT_FUN(V1C,V2C,DVC,k,V);
            }
        }
    }
  
}



// =================================================================================

// CKD version 2.2.2 H2O foreign continuum absorption model
void CKD_222_foreign_h2o( MatrixView          xsec,
                          const Numeric       Cin,
                          const String&       model,
                          ConstVectorView     f_mono,
                          ConstVectorView     p_abs,
                          ConstVectorView     t_abs,
                          ConstVectorView     vmr,
                          ConstVectorView     /* n2_abs */ )
{

  // check the model name about consistency
  if ((model != "user") &&  (model != "CKD222"))
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKDv2.2.2 H2O foreign continuum:\n"
         << "INPUT model name is: " << model << ".\n"
         << "VALID model names are user and CKD222\n";
      throw runtime_error(os.str());
    }


  // scaling factor of the foreign H2O cont. absorption
  Numeric  ScalingFac = 1.0000e0;
  if ( model == "user" )
    {
      ScalingFac = Cin; // input scaling factor of calculated absorption
    }


  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies


  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );


  // ************************** CKD stuff ************************************

  const Numeric xLosmt = 2.686763e19; // [molecules/cm^3]
  const Numeric T1     =  273.000e0;
  const Numeric TO     =  296.000e0;
  const Numeric PO     = 1013.000e0;

  // CKD2.2.2 foreign H2O continuum correction function parameters
  const Numeric HWSQF  = 330.000e0 * 330.000e0;
  const Numeric BETAF  = 8.000e-11;
  const Numeric V0F    = 1130.000e0;
  const Numeric FACTRF = 0.970e0;
  
  const Numeric V0F2   = 1900.000e0;
  const Numeric HWSQF2 = 150.000e0 * 150.000e0;
  const Numeric BETA2  = 3.000e-6;

  // wavenumber range where CKD H2O foreign continuum is valid
  const Numeric VABS_min = FH2O_ckd_0_v1; // [cm^-1]
  const Numeric VABS_max = FH2O_ckd_0_v2; // [cm^-1]


  // It is assumed here that f_mono is monotonically increasing with index!
  // In future change this return into a change of the loop over
  // the frequency f_mono. n_f_new < n_f
  Numeric V1ABS = f_mono[0]     / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  Numeric V2ABS = f_mono[n_f-1] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  if ( (V1ABS < VABS_min) || (V1ABS > VABS_max) ||
       (V2ABS < VABS_min) || (V2ABS > VABS_max) )
    {
      out3  << "WARNING:\n"
            << "  CKD2.2.2 H2O foreign continuum:\n"
            << "  input frequency vector exceeds range of model validity\n"
            << "  " << FH2O_ckd_0_v1 << "<->" << FH2O_ckd_0_v2 << "cm^-1\n";
    }


  // ---------------------- subroutine FRN296 ------------------------------

  // retrieve the appropriate array sequence of the foreign continuum
  // arrays of the CKD model.
  Numeric DVC = FH2O_ckd_0_dv;
  Numeric V1C = V1ABS - DVC;
  Numeric V2C = V2ABS + DVC;
  
  int I1 = (int) ((V1C-FH2O_ckd_0_v1) / FH2O_ckd_0_dv);
  if (V1C < FH2O_ckd_0_v1) I1 = -1;
  V1C = FH2O_ckd_0_v1 + (FH2O_ckd_0_dv * (Numeric)I1);

  int I2 = (int) ((V2C-FH2O_ckd_0_v1) / FH2O_ckd_0_dv);

  int NPTC = I2-I1+3;
  if (NPTC > FH2O_ckd_0_npt) NPTC = FH2O_ckd_0_npt+1;

  V2C = V1C + FH2O_ckd_0_dv * (Numeric)(NPTC-1);  
  
  if (NPTC < 1)
    {
      out3 << "WARNING:\n" 
           << "  CKD2.2.2 H2O foreign continuum:\n"
           << "  no elements of internal continuum coefficients could be found for the\n"
           << "  input frequency range.\n"
           << "  Leave the function without calculating the absorption.";
      return;
    }

  Numeric FH2OT0[NPTC+addF77fields]; // [cm^3/molecules]

  for (Index J = 1 ; J <= NPTC ; ++J)
    {
      Index I = I1+J;
      if ( (I < 1) || (I > FH2O_ckd_0_npt) ) 
        {
          FH2OT0[J] = 0.0e0;
        }
      else
        {
          FH2OT0[J] = FH2O_ckd_0[I];
        }
    }

  // ---------------------- subroutine FRN296 ------------------------------
  
  Numeric VF2   = 0.000e0;
  Numeric VF4   = 0.000e0;
  Numeric VF6   = 0.000e0;
  Numeric FSCAL = 0.000e0;
  Numeric FH2O  = 0.000e0;
  
  // Loop pressure/temperature:
  for ( Index i = 0 ; i < n_p ; ++i )
    {

      // atmospheric state parameters
      Numeric Tave   = t_abs[i];                               // [K]
      Numeric Pave   = (p_abs[i]*1.000e-2);                    // [hPa]
      Numeric vmrh2o = vmr[i];                                 // [1]
      // FIXME Numeric ph2o   = vmrh2o * Pave;                          // [hPa]
      Numeric PFRGN  = (Pave/PO) * (1.00000e0 - vmrh2o);       // dry air pressure [hPa]
      Numeric RFRGN  = PFRGN  * (TO/Tave);                     // [hPa]
      Numeric WTOT   = xLosmt * (Pave/PO) * (T1/Tave);         // [molecules/cm^2]
      // FIXME Numeric W1     = vmrh2o * WTOT;                          // [molecules/cm^2]
      Numeric XKT    = Tave   / 1.4387752;                     // = (T*k_B) / (h*c)
      
      // Molecular cross section calculated by CKD.
      // The cross sectionis calculated on the predefined 
      // CKD wavenumber grid.
      Numeric k[NPTC+addF77fields]; // [1/cm]
      k[0] = 0.00e0; // not used array field
      for (Index J = 1 ; J <= NPTC ; ++J)
        {
          Numeric VJ = V1C + (DVC * (Numeric)(J-1)); 

          // CORRECTION TO FOREIGN CONTINUUM
          VF2   = (VJ-V0F)  * (VJ-V0F);
          VF6   = VF2 * VF2 * VF2;
          FSCAL = (1.000e0 - FACTRF*(HWSQF/(VF2+(BETAF*VF6)+HWSQF)));

          VF2   = (VJ-V0F2) * (VJ-V0F2);
          VF4   = VF2 * VF2;
          FSCAL = FSCAL * (1.000e0 - 0.600e0*(HWSQF2/(VF2 + BETA2*VF4 + HWSQF2)));
     
          FH2O  = FH2OT0[J] * FSCAL;

          // CKD cross section with radiative field [1/cm]
          // The VMRH2O will be multiplied in absCalc, hence WTOT and not W1
          // as multiplicative term
          k[J] = WTOT * RFRGN * (FH2O*1.000e-20) * RADFN_FUN(VJ,XKT);

        }
      

      // Loop input frequency array. The previously calculated cross section 
      // has therefore to be interpolated on the input frequencies.
      for ( Index s = 0 ; s < n_f ; ++s )
        {
          // calculate the associated wave number (= 1/wavelength)
          Numeric V = f_mono[s] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
          if ( (V > 0.000e0) && (V < VABS_max) )
            {
              // arts CKD2.2.2 foreign H2O continuum cross section [1/m]
              // interpolate the k vector on the f_mono grid
              // The factor 100 comes from the conversion from (1/cm) to (1/m) 
              // of the abs. coeff.
              xsec(s,i) +=  ScalingFac * 1.000e2 * XINT_FUN(V1C,V2C,DVC,k,V);
            }
        }
    }
  
}


// =================================================================================

// CKD version 2.4.2 H2O self continuum absorption model
void CKD_242_self_h2o( MatrixView          xsec,
                       const Numeric       Cin,
                       const String&       model,
                       ConstVectorView     f_mono,
                       ConstVectorView     p_abs,
                       ConstVectorView     t_abs,
                       ConstVectorView     vmr,
                       ConstVectorView     /* n2_abs */ )
{


  // check the model name about consistency
  if ((model != "user") &&  (model != "CKD242"))
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKDv2.4.2 H2O self continuum:\n"
         << "INPUT model name is: " << model << ".\n"
         << "VALID model names are user and CKD242\n";
      throw runtime_error(os.str());
    }


  // scaling factor of the self H2O cont. absorption
  Numeric  ScalingFac = 1.0000e0;
  if ( model == "user" )
    {
      ScalingFac = Cin; // input scaling factor of calculated absorption
    }


  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies


  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );


  // ************************** CKD stuff ************************************

  const Numeric xLosmt   = 2.686763e19; // [molecules/cm^3]
  // FIXME const Numeric T1       =  273.0e0;
  const Numeric TO       =  296.0e0;
  const Numeric PO       = 1013.0e0;

  // CKD2.4.2 specific correction functions
  const Numeric V0S1     = 0.000e+00;
  const Numeric HWSQ1    = (1.000e+02 * 1.000e+02);
  const Numeric BETAS1   = 1.000e-04;
  const Numeric FACTRS1  = 0.688e+00;
  
  const Numeric V0S2     = 1.050e+03;
  const Numeric HWSQ2    = (2.000e+02 * 2.000e+02);
  const Numeric FACTRS2  = -0.2333e+00;
  
  const Numeric V0S3     = 1.310e+03;
  const Numeric HWSQ3    = (1.200e+02 * 1.200e+02);
  const Numeric BETAS3   = 5.000e-06;
  const Numeric FACTRS3  = -0.150e+00;
  
  const Numeric XFAC[51] = {  
    1.00000,1.01792,1.03767,1.05749,1.07730,1.09708,
    1.10489,1.11268,1.12047,1.12822,1.13597,1.14367,
    1.15135,1.15904,1.16669,1.17431,1.18786,1.20134,
    1.21479,1.22821,1.24158,1.26580,1.28991,1.28295,
    1.27600,1.26896,1.25550,1.24213,1.22879,1.21560,
    1.20230,1.18162,1.16112,1.14063,1.12016,1.10195,
    1.09207,1.08622,1.08105,1.07765,1.07398,1.06620,
    1.05791,1.04905,1.03976,1.02981,1.00985,1.00000,
    1.00000,1.00000,1.00000};

  // wavenumber range where CKD H2O self continuum is valid
  const Numeric VABS_min = SL260_ckd_0_v1; // [cm^-1]
  const Numeric VABS_max = SL260_ckd_0_v2; // [cm^-1]


  // It is assumed here that f_mono is monotonically increasing with index!
  // In future change this return into a change of the loop over
  // the frequency f_mono. n_f_new < n_f
  Numeric V1ABS = f_mono[0]     / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  Numeric V2ABS = f_mono[n_f-1] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  if ( (V1ABS < VABS_min) || (V1ABS > VABS_max) ||
       (V2ABS < VABS_min) || (V2ABS > VABS_max) )
    {
      out3  << "WARNING:\n"
            << "  CKD2.4.2 H2O self continuum:\n"
            << "  input frequency vector exceeds range of model validity\n"
            << "  " << SL296_ckd_0_v1 << "<->" << SL296_ckd_0_v2 << "cm^-1\n";
    }


  // ------------------- subroutine SL296/SL260 ----------------------------

  if (SL296_ckd_0_v1 != SL260_ckd_0_v1)
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD2.4.2 H2O self continuum:\n"
         << "parameter V1 not the same for different ref. temperatures.\n";
      throw runtime_error(os.str());
    }
  if (SL296_ckd_0_v2 != SL260_ckd_0_v2)
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD2.4.2 H2O self continuum:\n"
         << "parameter V2 not the same for different ref. temperatures.\n";
        throw runtime_error(os.str());
    }
  if (SL296_ckd_0_dv != SL260_ckd_0_dv)
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD2.4.2 H2O self continuum:\n"
         << "parameter DV not the same for different ref. temperatures.\n";
      throw runtime_error(os.str());
    }
  if (SL296_ckd_0_npt != SL260_ckd_0_npt)
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD2.4.2 H2O self continuum:\n"
         << "parameter NPT not the same for different ref. temperatures.\n";
      throw runtime_error(os.str());
    }
  
  // retrieve the appropriate array sequence of the self continuum
  // arrays of the CKD model.
  Numeric DVC = SL296_ckd_0_dv;
  Numeric V1C = V1ABS - DVC;
  Numeric V2C = V2ABS + DVC;
  
  int I1 = (int) ((V1C-SL296_ckd_0_v1) / SL296_ckd_0_dv);
  if (V1C < SL296_ckd_0_v1) I1 = -1;
  V1C = SL296_ckd_0_v1 + (SL296_ckd_0_dv * (Numeric)I1);

  int I2 = (int) ((V2C-SL296_ckd_0_v1) / SL296_ckd_0_dv);

  int NPTC = I2-I1+3;
  if (NPTC > SL296_ckd_0_npt) NPTC = SL296_ckd_0_npt+1;

  V2C = V1C + SL296_ckd_0_dv * (Numeric)(NPTC-1);  
  
  if (NPTC < 1)
    {
      ostringstream os;
      out3 << "WARNING:\n"  
           << "  CKDv2.4.2 H2O self continuum:\n"
           << "  no elements of internal continuum coefficients could be found for the\n"
           << "  input frequency range.\n"
           << "  Leave the function without calculating the absorption.";
      return;
    }

  Numeric SH2OT0[NPTC+addF77fields]; // [cm^3/molecules]
  Numeric SH2OT1[NPTC+addF77fields]; // [cm^3/molecules]

  for (Index J = 1 ; J <= NPTC ; ++J)
    {
      Index I = I1+J;
      if ( (I < 1) || (I > SL296_ckd_0_npt) ) 
        {
          SH2OT0[J] = 0.0e0;   // at T=296 K
          SH2OT1[J] = 0.0e0;   // at T=260 K
        }
      else
        {
          SH2OT0[J] = SL296_ckd_0[I];    // at T=296 K
          SH2OT1[J] = SL260_ckd_0[I];    // at T=260 K 
        }
    }

  // ------------------- subroutine SL296/SL260 ----------------------------
  
  Numeric SFAC = 1.00e0;
  Numeric VS2  = 0.00e0;
  Numeric VS4  = 0.00e0;
  
  // Loop pressure/temperature:
  for ( Index i = 0 ; i < n_p ; ++i )
    {

      // atmospheric state parameters
      Numeric Tave   = t_abs[i];                                     // [K]
      Numeric Pave   = (p_abs[i]*1.000e-2);                          // [hPa]
      Numeric Patm   = Pave/PO;                                      // [1]
      Numeric vmrh2o = vmr[i];                                       // [1]
      // FIXME Numeric Ph2o   = Patm * vmrh2o;                                // [1]
      // second vmr in absCalc multiplied
      Numeric Rh2o   = Patm * (TO/Tave);                             // [1]
      Numeric Tfac   = (Tave-TO)/(260.0-TO);                         // [1]
      Numeric WTOT   = xLosmt * (Pave/1.013000e3) * (2.7300e2/Tave); // [molecules/cm^2]
      Numeric W1     = vmrh2o * WTOT;                                // [molecules/cm^2]
      Numeric XKT    = Tave / 1.4387752e0;                           // = (T*k_B)/(h*c)   
      
      // Molecular cross section calculated by CKD.
      // The cross sectionis calculated on the predefined 
      // CKD wavenumber grid.
      Numeric k[NPTC+addF77fields]; // [1/cm]
      k[0] = 0.00e0; // not used array field
      for (Index J = 1 ; J <= NPTC ; ++J)
        {
          Numeric VJ   = V1C + (DVC * (Numeric)(J-1)); 
          Numeric SH2O = 0.0e0;
          if (SH2OT0[J] > 0.0e0)
            {
              SH2O = SH2OT0[J] * pow( (SH2OT1[J]/SH2OT0[J]), Tfac ); 
              SFAC = 1.00e0;

              if ( (VJ >= 700.0e0) && (VJ <= 1200.0e0) )
                {
                  int JFAC = (int)((VJ - 700.0e0)/10.0e0 + 0.00001e0);
                  if ( (JFAC >= 0) && (JFAC <= 50) )
                    SFAC = XFAC[JFAC];
                }

              // ---------------------------------------------------------
              // Correction to self continuum (1 SEPT 85); factor of    
              // 0.78 at 1000 and  .......

              VS2  = (VJ-V0S1) * (VJ-V0S1);
              VS4  = VS2*VS2;
              SFAC = SFAC * 
                (1.000e0 + FACTRS1*(HWSQ1/((VJ*VJ)+(BETAS1*VS4)+HWSQ1))); 

              VS2  = (VJ-V0S2) * (VJ-V0S2);
              SFAC = SFAC *
                (1.000e0 + FACTRS2*(HWSQ2/(VS2+HWSQ2)));

              VS2  = (VJ-V0S3) * (VJ-V0S3);
              VS4  = VS2*VS2;
              SFAC = SFAC *
                (1.000e0 + FACTRS3*(HWSQ3/(VS2+(BETAS3*VS4)+HWSQ3))); 
              
              SH2O = SFAC * SH2O;
            }

          // CKD cross section with radiative field [1/cm]
          // The VMRH2O will be multiplied in absCalc, hence Rh2o does not contain 
          // VMRH2O as multiplicative term
          k[J] = W1 * Rh2o * (SH2O*1.000e-20) * RADFN_FUN(VJ,XKT);

        }
      

      // Loop input frequency array. The previously calculated cross section 
      // has therefore to be interpolated on the input frequencies.
      for ( Index s = 0 ; s < n_f ; ++s )
        {
          // calculate the associated wave number (= 1/wavelength)
          Numeric V = f_mono[s] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
          if ( (V >= 0.000e0) && (V < SL296_ckd_0_v2) )
            {
              // arts cross section [1/m]
              // interpolate the k vector on the f_mono grid
              // The factor 100 comes from the conversion from 1/cm to 1/m for
              // the absorption coefficient
              xsec(s,i) +=  ScalingFac * 1.000e2 * XINT_FUN(V1C,V2C,DVC,k,V);
            }
        }
    }
  
}


// =================================================================================

// CKD version 2.4.2 H2O foreign continuum absorption model
void CKD_242_foreign_h2o( MatrixView          xsec,
                          const Numeric       Cin,
                          const String&       model,
                          ConstVectorView     f_mono,
                          ConstVectorView     p_abs,
                          ConstVectorView     t_abs,
                          ConstVectorView     vmr,
                          ConstVectorView     /* n2_abs */ )
{


  // check the model name about consistency
  if ((model != "user") &&  (model != "CKD242"))
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKDv2.4.2 H2O foreign continuum:\n"
         << "INPUT model name is: " << model << ".\n"
         << "VALID model names are user and CKD242\n";
      throw runtime_error(os.str());
    }


  // scaling factor of the foreign H2O cont. absorption
  Numeric  ScalingFac = 1.0000e0;
  if ( model == "user" )
    {
      ScalingFac = Cin; // input scaling factor of calculated absorption
    }


  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );


  // ************************** CKD stuff ************************************

  const Numeric xLosmt = 2.686763e19; // [molecules/cm^3]
  const Numeric T1     =  273.0e0;
  const Numeric TO     =  296.0e0;
  const Numeric PO     = 1013.0e0;

  // CKD2.4.2 foreign H2O continuum correction function parameters
  const Numeric V0F1     = 350.000e0;
  const Numeric HWSQF1   = 200.000e0 * 200.000e0;
  const Numeric BETAF1   = 5.000e-9 ;
  const Numeric FACTRF1  = -0.700e0;
  
  const Numeric V0F1a    = 630.000e0;
  const Numeric HWSQF1a  = 65.000e0*65.000e0;
  const Numeric BETAF1a  = 2.000e-08 ;
  const Numeric FACTRF1a = 0.750e0;
  
  const Numeric V0F2     = 1130.000e0;
  const Numeric HWSQF2   = 330.000e0 * 330.000e0;
  const Numeric BETAF2   = 8.000e-11;
  const Numeric FACTRF2  = -0.970e0;
  
  const Numeric V0F3     = 1975.000e0;
  const Numeric HWSQF3   = 250.000e0 * 250.000e0;
  const Numeric BETAF3   = 5.000e-06;
  const Numeric FACTRF3  = -0.650e0;

  // wavenumber range where CKD H2O foreign continuum is valid
  const Numeric VABS_min = FH2O_ckd_0_v1; // [cm^-1]
  const Numeric VABS_max = FH2O_ckd_0_v2; // [cm^-1]


  // It is assumed here that f_mono is monotonically increasing with index!
  // In future change this return into a change of the loop over
  // the frequency f_mono. n_f_new < n_f
  Numeric V1ABS = f_mono[0]     / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  Numeric V2ABS = f_mono[n_f-1] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  if ( (V1ABS < VABS_min) || (V1ABS > VABS_max) ||
       (V2ABS < VABS_min) || (V2ABS > VABS_max) )
    {
      out3  << "WARNING:\n"
            << "  CKDv2.4.2 H2O foreign continuum:\n"
            << "  input frequency vector exceeds range of model validity\n"
            << "  " << FH2O_ckd_0_v1 << "<->" << FH2O_ckd_0_v2 << "cm^-1\n";
    }


  // ---------------------- subroutine FRN296 ------------------------------

  // retrieve the appropriate array sequence of the foreign continuum
  // arrays of the CKD model.
  Numeric DVC = FH2O_ckd_0_dv;
  Numeric V1C = V1ABS - DVC;
  Numeric V2C = V2ABS + DVC;
  
  int I1 = (int) ((V1C-FH2O_ckd_0_v1) / FH2O_ckd_0_dv);
  if (V1C < FH2O_ckd_0_v1) I1 = -1;
  V1C = FH2O_ckd_0_v1 + (FH2O_ckd_0_dv * (Numeric)I1);

  int I2 = (int) ((V2C-FH2O_ckd_0_v1) / FH2O_ckd_0_dv);

  int NPTC = I2-I1+3;
  if (NPTC > FH2O_ckd_0_npt) NPTC = FH2O_ckd_0_npt+1;

  V2C = V1C + FH2O_ckd_0_dv * (Numeric)(NPTC-1);  
  
  if (NPTC < 1)
    {
      out3 << "WARNING:\n" 
           << "  CKDv2.4.2 H2O foreign continuum:\n"
           << "  no elements of internal continuum coefficients could be found for the\n"
           << "  input frequency range.\n"
           << "  Leave the function without calculating the absorption.";
      return;
    }

  Numeric FH2OT0[NPTC+addF77fields]; // [cm^3/molecules]

  for (Index J = 1 ; J <= NPTC ; ++J)
    {
      Index I = I1+J;
      if ( (I < 1) || (I > FH2O_ckd_0_npt) ) 
        {
          FH2OT0[J] = 0.0e0;
        }
      else
        {
          FH2OT0[J] = FH2O_ckd_0[I];
        }
    }

  // ---------------------- subroutine FRN296 ------------------------------
  
  Numeric VF2   = 0.000e0;
  Numeric VF4   = 0.000e0;
  Numeric VF6   = 0.000e0;
  Numeric FSCAL = 0.000e0;
  Numeric FH2O  = 0.000e0;
  
  // Loop pressure/temperature:
  for ( Index i = 0 ; i < n_p ; ++i )
    {

      // atmospheric state parameters
      Numeric Tave   = t_abs[i];                               // [K]
      Numeric Pave   = (p_abs[i]*1.000e-2);                    // [hPa]
      Numeric vmrh2o = vmr[i];                                 // [1]
      // FIXME Numeric ph2o   = vmrh2o * Pave;                          // [hPa]
      Numeric PFRGN  = (Pave/PO) * (1.00000e0 - vmrh2o);       // dry air pressure [hPa]
      Numeric RFRGN  = PFRGN  * (TO/Tave);                     // [hPa]
      Numeric WTOT   = xLosmt * (Pave/PO) * (T1/Tave);         // [molecules/cm^2]
      // FIXME Numeric W1     = vmrh2o * WTOT;                          // [molecules/cm^2]
      Numeric XKT    = Tave   / 1.4387752;                     // = (T*k_B) / (h*c)    
      
      // Molecular cross section calculated by CKD.
      // The cross sectionis calculated on the predefined 
      // CKD wavenumber grid.
      Numeric k[NPTC+addF77fields]; // [1/cm]
      k[0] = 0.00e0; // not used array field
      for (Index J = 1 ; J <= NPTC ; ++J)
        {
          Numeric VJ = V1C + (DVC * (Numeric)(J-1)); 

          // CORRECTION TO FOREIGN CONTINUUM
          VF2   = (VJ-V0F1) * (VJ-V0F1);
          VF6   = VF2 * VF2 * VF2;
          FSCAL = (1.000e0 + FACTRF1*(HWSQF1/(VF2+(BETAF1*VF6)+HWSQF1)));

          VF2   = (VJ-V0F1a) * (VJ-V0F1a);
          VF6   = VF2 * VF2  * VF2;
          FSCAL = FSCAL * 
                  (1.000e0 + FACTRF1a*(HWSQF1a/(VF2+(BETAF1a*VF6)+HWSQF1a)));

          VF2   = (VJ-V0F2) * (VJ-V0F2);
          VF6   = VF2 * VF2 * VF2;
          FSCAL = FSCAL * 
                  (1.000e0 + FACTRF2*(HWSQF2/(VF2+(BETAF2*VF6)+HWSQF2)));

          VF2   = (VJ-V0F3) * (VJ-V0F3);
          VF4   = VF2 * VF2;
          FSCAL = FSCAL * 
                  (1.000e0 + FACTRF3*(HWSQF3/(VF2+BETAF3*VF4+HWSQF3)));
     
          FH2O  = FH2OT0[J] * FSCAL;

          // CKD cross section without radiative field
          // The VMRH2O will be multiplied in absCalc, hence WTOT and not W1
          // as multiplicative term
          k[J] = WTOT * RFRGN * (FH2O*1.000e-20) * RADFN_FUN(VJ,XKT);

        }
      

      // Loop input frequency array. The previously calculated cross section 
      // has therefore to be interpolated on the input frequencies.
      for ( Index s = 0 ; s < n_f ; ++s )
        {
          // calculate the associated wave number (= 1/wavelength)
          Numeric V = f_mono[s] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
          if ( (V >= 0.000e0) && (V < VABS_max) )
            {
              // arts CKD2.4.2 foreign H2O continuum cross section [1/m]
              // interpolate the k vector on the f_mono grid
              xsec(s,i) +=  ScalingFac * 1.000e2 * XINT_FUN(V1C,V2C,DVC,k,V);
            }
        }
    }
  
}


// =================================================================================

// CKD version MT 1.00 H2O self continuum absorption model
void CKD_mt_100_self_h2o( MatrixView          xsec,
                          const Numeric       Cin,
                          const String&       model,
                          ConstVectorView     f_mono,
                          ConstVectorView     p_abs,
                          ConstVectorView     t_abs,
                          ConstVectorView     vmr,
                          ConstVectorView     /* n2_abs */ )
{

  // check the model name about consistency
  if ((model != "user") &&  (model != "CKDMT100"))
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD_MT1.00 H2O self continuum:\n"
         << "INPUT model name is: " << model << ".\n"
         << "VALID model names are user and CKDMT100\n";
      throw runtime_error(os.str());
    }


  // scaling factor of the self H2O cont. absorption
  Numeric  ScalingFac = 1.0000e0;
  if ( model == "user" )
    {
      ScalingFac = Cin; // input scaling factor of calculated absorption
    }


  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies


  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );


  // ************************** CKD stuff ************************************

  const Numeric xLosmt =    2.68675e19; // [molecules/cm^3]
  // FIXME const Numeric T1     =  273.000e0;    // [K]
  const Numeric TO     =  296.000e0;    // [K]
  const Numeric PO     = 1013.000e0;    // [hPa]

  const Numeric XFACREV[15] = 
    {1.003, 1.009, 1.015, 1.023, 1.029,1.033,
     1.037, 1.039, 1.040, 1.046, 1.036,1.027,
     1.01,  1.002, 1.00};

  // wavenumber range where CKD H2O self continuum is valid
  const Numeric VABS_min = -2.000e1; // [cm^-1]
  const Numeric VABS_max =  2.000e4; // [cm^-1]


  // It is assumed here that f_mono is monotonically increasing with index!
  // In future change this return into a change of the loop over
  // the frequency f_mono. n_f_new < n_f
  Numeric V1ABS = f_mono[0]     / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  Numeric V2ABS = f_mono[n_f-1] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  if ( (V1ABS < VABS_min) || (V1ABS > VABS_max) ||
       (V2ABS < VABS_min) || (V2ABS > VABS_max) )
    {
      out3  << "WARNING:\n"
            << "  CKD_MT 1.00 H2O self continuum:\n"
            << "  input frequency vector exceeds range of model validity\n"
            << "  " << SL296_ckd_mt_100_v1 << "<->" << SL296_ckd_mt_100_v2 << "cm^-1\n";
    }


  // ------------------- subroutine SL296/SL260 ----------------------------

  if (SL296_ckd_mt_100_v1 != SL260_ckd_mt_100_v1)
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD_MT 1.00 H2O self continuum:\n"
         << "parameter V1 not the same for different ref. temperatures.\n";
      throw runtime_error(os.str());
    }
  if (SL296_ckd_mt_100_v2 != SL260_ckd_mt_100_v2)
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD_MT 1.00 H2O self continuum:\n"
         << "parameter V2 not the same for different ref. temperatures.\n";
        throw runtime_error(os.str());
    }
  if (SL296_ckd_mt_100_dv != SL260_ckd_mt_100_dv)
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD_MT 1.00 H2O self continuum:\n"
         << "parameter DV not the same for different ref. temperatures.\n";
      throw runtime_error(os.str());
    }
  if (SL296_ckd_mt_100_npt != SL260_ckd_mt_100_npt)
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD_MT 1.00 H2O self continuum:\n"
         << "parameter NPT not the same for different ref. temperatures.\n";
      throw runtime_error(os.str());
    }
  
  // retrieve the appropriate array sequence of the self continuum
  // arrays of the CKD model.
  Numeric DVC = SL296_ckd_mt_100_dv;
  Numeric V1C = V1ABS - DVC;
  Numeric V2C = V2ABS + DVC;
  
  int I1 = (int) ((V1C-SL296_ckd_mt_100_v1) / SL296_ckd_mt_100_dv);
  if (V1C < SL296_ckd_mt_100_v1) I1 = -1;
  V1C = SL296_ckd_mt_100_v1 + (SL296_ckd_mt_100_dv * (Numeric)I1);

  int I2 = (int) ((V2C-SL296_ckd_mt_100_v1) / SL296_ckd_mt_100_dv);

  int NPTC = I2-I1+3;
  if (NPTC > SL296_ckd_mt_100_npt) NPTC = SL296_ckd_mt_100_npt+1;

  V2C = V1C + SL296_ckd_mt_100_dv * (Numeric)(NPTC-1);  
  
  if (NPTC < 1)
    {
      ostringstream os;
      out3 << "WARNING:\n"  
           << "  CKD_MT 1.00 H2O self continuum:\n"
           << "  no elements of internal continuum coefficients could be found for the\n"
           << "  input frequency range.\n"
           << "  Leave the function without calculating the absorption.";
      return;
    }

  Numeric SH2OT0[NPTC+addF77fields]; // [cm^3/molecules]
  Numeric SH2OT1[NPTC+addF77fields]; // [cm^3/molecules]

  for (Index J = 1 ; J <= NPTC ; ++J)
    {
      Index I = I1+J;
      if ( (I < 1) || (I > SL296_ckd_mt_100_npt) ) 
        {
          SH2OT0[J] = 0.0e0;   // at T=296 K
          SH2OT1[J] = 0.0e0;   // at T=260 K
        }
      else
        {
          SH2OT0[J] = SL296_ckd_mt_100[I];    // at T=296 K
          SH2OT1[J] = SL260_ckd_mt_100[I];    // at T=260 K 
        }
    }

  // ------------------- subroutine SL296/SL260 ----------------------------
  
  Numeric SFAC = 1.00e0;  

  // Loop pressure/temperature:
  for ( Index i = 0 ; i < n_p ; ++i )
    {

      // atmospheric state parameters
      Numeric Tave   = t_abs[i];                                     // [K]
      Numeric Pave   = (p_abs[i]*1.000e-2);                          // [hPa]
      Numeric Patm   = Pave/PO;                                      // [1]
      Numeric vmrh2o = vmr[i];                                       // [1]
      // FIXME Numeric Ph2o   = Patm * vmrh2o;                                // [1]
      // second vmr in absCalc multiplied
      Numeric Rh2o   = Patm * (TO/Tave);                             // [1]
      Numeric Tfac   = (Tave-TO)/(260.0-TO);                         // [1]
      Numeric WTOT   = xLosmt * (Pave/1.013000e3) * (2.7300e2/Tave); // [molecules/cm^2]
      Numeric W1     = vmrh2o * WTOT;                                // [molecules/cm^2]
      Numeric XKT    = Tave / 1.4387752e0;                           // = (T*k_B)/(h*c)    

      // Molecular cross section calculated by CKD.
      // The cross sectionis calculated on the predefined 
      // CKD wavenumber grid.
      Numeric k[NPTC+addF77fields]; // [1/cm]
      k[0] = 0.00e0; // not used array field
      for (Index J = 1 ; J <= NPTC ; ++J)
        {
          Numeric VJ   = V1C + (DVC * (Numeric)(J-1)); 
          Numeric SH2O = 0.0e0;
          if (SH2OT0[J] > 0.0e0)
            {
              SH2O = SH2OT0[J] * pow( (SH2OT1[J]/SH2OT0[J]), Tfac ); 
              SFAC = 1.00e0;

              if ( (VJ >= 820.0e0) && (VJ <= 960.0e0) )
                {
                  int JFAC = (int)((VJ - 820.0e0)/10.0e0 + 0.00001e0);
                  if ( (JFAC >= 0) && (JFAC <=14) )
                    SFAC = XFACREV[JFAC];
                }

              SH2O = SFAC * SH2O;
            }

          // CKD cross section with radiative field [1/cm]
          // The VMRH2O will be multiplied in absCalc, hence Rh2o does not contain 
          // VMRH2O as multiplicative term
          k[J] = W1 * Rh2o * (SH2O*1.000e-20) * RADFN_FUN(VJ,XKT);

        }
      

      // Loop input frequency array. The previously calculated cross section 
      // has therefore to be interpolated on the input frequencies.
      for ( Index s = 0 ; s < n_f ; ++s )
        {
          // calculate the associated wave number (= 1/wavelength)
          Numeric V = f_mono[s] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
          if ( (V > 0.000e0) && (V < SL296_ckd_mt_100_v2) )
            {
              // arts cross section [1/m]
              // interpolate the k vector on the f_mono grid
              // The factor 100 comes from the conversion from 1/cm to 1/m for
              // the absorption coefficient
              xsec(s,i) +=  ScalingFac * 1.000e2 * XINT_FUN(V1C,V2C,DVC,k,V);
            }
        }
    }
  
}

// =================================================================================

// CKD version MT 1.00 H2O foreign continuum absorption model
void CKD_mt_100_foreign_h2o( MatrixView          xsec,
                             const Numeric       Cin,
                             const String&       model,
                             ConstVectorView     f_mono,
                             ConstVectorView     p_abs,
                             ConstVectorView     t_abs,
                             ConstVectorView     vmr,
                             ConstVectorView     /* n2_abs */ )
{


  // check the model name about consistency
  if ((model != "user") &&  (model != "CKDMT100"))
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD_MT1.00 H2O foreign continuum:\n"
         << "INPUT model name is: " << model << ".\n"
         << "VALID model names are user and CKDMT100\n";
      throw runtime_error(os.str());
    }


  // scaling factor of the foreign H2O cont. absorption
  Numeric  ScalingFac = 1.0000e0;
  if ( model == "user" )
    {
      ScalingFac = Cin; // input scaling factor of calculated absorption
    }


  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies


  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );


  // ************************** CKD stuff ************************************

  const Numeric xLosmt = 2.68675e19; // [molecules/cm^3]
  const Numeric T1     =  273.000e0;
  const Numeric TO     =  296.000e0;
  const Numeric PO     = 1013.000e0;

  // wavenumber range where CKD H2O self continuum is valid
  const Numeric VABS_min = -2.000e1; // [cm^-1]
  const Numeric VABS_max =  2.000e4; // [cm^-1]


  // It is assumed here that f_mono is monotonically increasing with index!
  // In future change this return into a change of the loop over
  // the frequency f_mono. n_f_new < n_f
  Numeric V1ABS = f_mono[0]     / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  Numeric V2ABS = f_mono[n_f-1] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  if ( (V1ABS < VABS_min) || (V1ABS > VABS_max) ||
       (V2ABS < VABS_min) || (V2ABS > VABS_max) )
    {
      out3  << "WARNING:\n"
            << "  CKD_MT 1.00 H2O foreign continuum:\n"
            << "  input frequency vector exceeds range of model validity\n"
            << "  " << FH2O_ckd_mt_100_v1 << "<->" << FH2O_ckd_mt_100_v2 << "cm^-1\n";
    }


  // ---------------------- subroutine FRN296 ------------------------------

  // retrieve the appropriate array sequence of the foreign continuum
  // arrays of the CKD model.
  Numeric DVC = FH2O_ckd_mt_100_dv;
  Numeric V1C = V1ABS - DVC;
  Numeric V2C = V2ABS + DVC;
  
  int I1 = (int) ((V1C-FH2O_ckd_mt_100_v1) / FH2O_ckd_mt_100_dv);
  if (V1C < FH2O_ckd_mt_100_v1) I1 = -1;
  V1C = FH2O_ckd_mt_100_v1 + (FH2O_ckd_mt_100_dv * (Numeric)I1);

  int I2 = (int) ((V2C-FH2O_ckd_mt_100_v1) / FH2O_ckd_mt_100_dv);

  int NPTC = I2-I1+3;
  if (NPTC > FH2O_ckd_mt_100_npt) NPTC = FH2O_ckd_mt_100_npt+1;

  V2C = V1C + FH2O_ckd_mt_100_dv * (Numeric)(NPTC-1);  
  
  if (NPTC < 1)
    {
      out3 << "WARNING:\n" 
           << "  CKD_MT 1.00 H2O foreign continuum:\n"
           << "  no elements of internal continuum coefficients could be found for the\n"
           << "  input frequency range.\n"
           << "  Leave the function without calculating the absorption.";
      return;
    }

  Numeric FH2OT0[NPTC+addF77fields]; // [cm^3/molecules]

  for (Index J = 1 ; J <= NPTC ; ++J)
    {
      Index I = I1+J;
      if ( (I < 1) || (I > FH2O_ckd_mt_100_npt) ) 
        {
          FH2OT0[J] = 0.0e0;
        }
      else
        {
          FH2OT0[J] = FH2O_ckd_mt_100[I];
        }
    }

  // ---------------------- subroutine FRN296 ------------------------------
  
  


  // Loop pressure/temperature:
  for ( Index i = 0 ; i < n_p ; ++i )
    {
      // atmospheric state parameters
      Numeric Tave   = t_abs[i];                               // [K]
      Numeric Pave   = (p_abs[i]*1.000e-2);                    // [hPa]
      Numeric vmrh2o = vmr[i];                                 // [1]
      // FIXME Numeric ph2o   = vmrh2o * Pave;                          // [hPa]
      Numeric PFRGN  = (Pave/PO) * (1.00000e0 - vmrh2o);       // dry air pressure [hPa]
      Numeric RFRGN  = PFRGN  * (TO/Tave);                     // [hPa]
      Numeric WTOT   = xLosmt * (Pave/PO) * (T1/Tave);         // [molecules/cm^2]
      // FIXME Numeric W1     = vmrh2o * WTOT;                          // [molecules/cm^2]
      Numeric XKT    = Tave   / 1.4387752;                     // = (T*k_B) / (h*c)    
      
      // Molecular cross section calculated by CKD.
      // The cross sectionis calculated on the predefined 
      // CKD wavenumber grid.
      Numeric k[NPTC+addF77fields]; // [1/cm]
      k[0] = 0.00e0; // not used array field
      for (Index J = 1 ; J <= NPTC ; ++J)
        {
          Numeric VJ   = V1C + (DVC * (Numeric)(J-1)); 
          Numeric FH2O = FH2OT0[J];

          // CKD cross section with radiative field [1/cm]
          // The VMRH2O will be multiplied in absCalc, hence WTOT and not W1
          // as multiplicative term
          k[J] = WTOT * RFRGN * (FH2O*1.000e-20) * RADFN_FUN(VJ,XKT);

        }
      
      // Loop input frequency array. The previously calculated cross section 
      // has therefore to be interpolated on the input frequencies.
      for ( Index s = 0 ; s < n_f ; ++s )
        {
          // calculate the associated wave number (= 1/wavelength)
          Numeric V = f_mono[s] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
          if ( (V >= 0.000e0) && (V < VABS_max) )
            {
              // arts CKD_MT.100 cross section [1/m]
              // interpolate the k vector on the f_mono grid
              // The factor 100 comes from the conversion from (1/cm) to (1/m) 
              // of the abs. coeff.
              xsec(s,i) +=  ScalingFac * 1.000e2 * XINT_FUN(V1C,V2C,DVC,k,V);
            }
        }
    }
  
}

//

// =================================================================================

// CKD version 2.4.1 CO2 continuum absorption model
void CKD_241_co2( MatrixView         xsec,
                 const Numeric       Cin,
                 const String&       model,
                 ConstVectorView     f_mono,
                 ConstVectorView     p_abs,
                 ConstVectorView     t_abs,
                 ConstVectorView     vmr )
{

  // check the model name about consistency
  if ((model != "user") &&  (model != "CKD241"))
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKDv2.4.1 CO2 continuum:\n"
         << "INPUT model name is: " << model << ".\n"
         << "VALID model names are user and CKD241\n";
      throw runtime_error(os.str());
    }


  // scaling factor of the CO2 absorption
  Numeric  ScalingFac = 0.0000e0;
  if ( model == "user" )
    {
      ScalingFac = Cin; // input scaling factor of calculated absorption
    }
  else
    {
      ScalingFac = 1.0000e0;
    }

  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies


  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );


  // ************************** CKD stuff ************************************

  const Numeric xLosmt = 2.686763e19; // [molecules/cm^3]
  const Numeric T1     =  273.0e0;
  const Numeric TO     =  296.0e0;
  const Numeric PO     = 1013.0e0;

  // wavenumber range where CKD CO2 continuum is valid
  const Numeric VABS_min = -2.000e1; // [cm^-1]
  const Numeric VABS_max =  1.000e4; // [cm^-1]


  // It is assumed here that f_mono is monotonically increasing with index!
  // In future change this return into a change of the loop over
  // the frequency f_mono. n_f_new < n_f
  Numeric V1ABS = f_mono[0]     / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  Numeric V2ABS = f_mono[n_f-1] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  if ( (V1ABS < VABS_min) || (V1ABS > VABS_max) ||
       (V2ABS < VABS_min) || (V2ABS > VABS_max) )
    {
      out3  << "WARNING:\n"
            << "  CKDv2.4.1 CO2 continuum:\n"
            << "  input frequency vector exceeds range of model validity\n"
            << "  " << FCO2_ckd_mt_100_v1 << "<->" << FCO2_ckd_mt_100_v2 << "cm^-1\n";
    }


  // ---------------------- subroutine FRNCO2 ------------------------------

  // retrieve the appropriate array sequence of the CO2 continuum
  // arrays of the CKD model.
  Numeric DVC = FCO2_ckd_mt_100_dv;
  Numeric V1C = V1ABS - DVC;
  Numeric V2C = V2ABS + DVC;
  
  int I1 = (int) ((V1C-FCO2_ckd_mt_100_v1) / FCO2_ckd_mt_100_dv);
  if (V1C < FCO2_ckd_mt_100_v1) I1 = -1;
  V1C = FCO2_ckd_mt_100_v1 + (FCO2_ckd_mt_100_dv * (Numeric)I1);

  int I2 = (int) ((V2C-FCO2_ckd_mt_100_v1) / FCO2_ckd_mt_100_dv);

  int NPTC = I2-I1+3;
  if (NPTC > FCO2_ckd_mt_100_npt) NPTC = FCO2_ckd_mt_100_npt+1;

  V2C = V1C + FCO2_ckd_mt_100_dv * (Numeric)(NPTC-1);  
  
  if (NPTC < 1)
    {
      out3 << "WARNING:\n"  
           << "  CKDv2.4.1 CO2 continuum:\n"
           << "  no elements of internal continuum coefficients could be found for the\n"
           << "  input frequency range.\n"
           << "  Leave the function without calculating the absorption.";
      return;
    }

  Numeric FCO2T0[NPTC+addF77fields]; // [cm^3/molecules]

  for (Index J = 1 ; J <= NPTC ; ++J)
    {
      Index I = I1+J;
      if ( (I < 1) || (I > FCO2_ckd_mt_100_npt) ) 
        {
          FCO2T0[J] = 0.0e0;
        }
      else
        {
          FCO2T0[J] = FCO2_ckd_mt_100[I];
        }
    }

  // ---------------------- subroutine FRNCO2 ------------------------------
  
  


  // Loop pressure/temperature:
  for ( Index i = 0 ; i < n_p ; ++i )
    {
      Numeric Tave   = t_abs[i];                               // [K]
      Numeric Pave   = (p_abs[i]*1.000e-2);                    // [hPa]
      // FIXME Numeric vmrco2 = vmr[i];                                 // [1]
      Numeric Rhoave = (Pave/PO) * (TO/Tave);                  // [hPa]
      Numeric WTOT   = xLosmt * (Pave/PO) * (T1/Tave);         // [molecules/cm^2]
      Numeric XKT    = Tave / 1.4387752;                       // = (T*k_B) / (h*c)    
      

      // Molecular cross section calculated by CKD.
      // The cross sectionis calculated on the predefined 
      // CKD wavenumber grid.
      Numeric k[NPTC+addF77fields]; // [1/cm]
      k[0] = 0.00e0; // not used array field
      for (Index J = 1 ; J <= NPTC ; ++J)
        {
          Numeric VJ   = V1C + (DVC * (Numeric)(J-1)); 
          Numeric FCO2 = FCO2T0[J];

          // CKD cross section times number density with radiative field [1]
          // the VMRCO2 will be multiplied in absCalc
          k[J] = ((WTOT * Rhoave) * (FCO2*1.000e-20) * RADFN_FUN(VJ,XKT));

        }
      

      // Loop input frequency array. The previously calculated cross section 
      // has therefore to be interpolated on the input frequencies.
      for ( Index s = 0 ; s < n_f ; ++s )
        {
          // calculate the associated wave number (= 1/wavelength)
          Numeric V = f_mono[s] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
          if ( (V > 0.000e0) && (V < FCO2_ckd_mt_100_v2) )
            {
              // arts cross section [1/m]
              // interpolate the k vector on the f_mono grid
              xsec(s,i) +=  ScalingFac * 1.000e2 * XINT_FUN(V1C,V2C,DVC,k,V);
            }
        }
    }
  
}


// =================================================================================


// CKD version MT 1.00 CO2 continuum absorption model
void CKD_mt_co2( MatrixView          xsec,
                 const Numeric       Cin,
                 const String&       model,
                 ConstVectorView     f_mono,
                 ConstVectorView     p_abs,
                 ConstVectorView     t_abs,
                 ConstVectorView     vmr)
{


  // check the model name about consistency
  if ((model != "user") &&  (model != "CKDMT100"))
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD_MT.1.00 CO2 continuum:\n"
         << "INPUT model name is: " << model << ".\n"
         << "VALID model names are user and CKDMT100\n";
      throw runtime_error(os.str());
    }


  // scaling factor of the CO2 absorption
  Numeric  ScalingFac = 0.0000e0;
  if ( model == "user" )
    {
      ScalingFac = Cin; // input scaling factor of calculated absorption
    }
  else
    {
      ScalingFac = 1.0000e0;
    }

  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies


  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );


  // ************************** CKD stuff ************************************

  const Numeric xLosmt = 2.686763e19; // [molecules/cm^3]
  const Numeric T1     =  273.0e0;
  const Numeric TO     =  296.0e0;
  const Numeric PO     = 1013.0e0;

  // wavenumber range where CKD CO2 continuum is valid
  const Numeric VABS_min = FCO2_ckd_mt_100_v1; // [cm^-1]
  const Numeric VABS_max = FCO2_ckd_mt_100_v2; // [cm^-1]


  // It is assumed here that f_mono is monotonically increasing with index!
  // In future change this return into a change of the loop over
  // the frequency f_mono. n_f_new < n_f
  Numeric V1ABS = f_mono[0]     / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  Numeric V2ABS = f_mono[n_f-1] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  if ( (V1ABS < VABS_min) || (V1ABS > VABS_max) ||
       (V2ABS < VABS_min) || (V2ABS > VABS_max) )
    {
      out3  << "WARNING:\n"
            << "  CKD_MT 1.00 CO2 continuum:\n"
            << "  input frequency vector exceeds range of model validity\n"
            << "  " << FCO2_ckd_mt_100_v1 << "<->" << FCO2_ckd_mt_100_v2 << "cm^-1\n";
    }


  // ---------------------- subroutine FRNCO2 ------------------------------

  // retrieve the appropriate array sequence of the CO2 continuum
  // arrays of the CKD model.
  Numeric DVC = FCO2_ckd_mt_100_dv;
  Numeric V1C = V1ABS - DVC;
  Numeric V2C = V2ABS + DVC;
  
  int I1 = (int) ((V1C-FCO2_ckd_mt_100_v1) / FCO2_ckd_mt_100_dv);
  if (V1C < FCO2_ckd_mt_100_v1) I1 = -1;
  V1C = FCO2_ckd_mt_100_v1 + (FCO2_ckd_mt_100_dv * (Numeric)I1);

  int I2 = (int) ((V2C-FCO2_ckd_mt_100_v1) / FCO2_ckd_mt_100_dv);

  int NPTC = I2-I1+3;
  if (NPTC > FCO2_ckd_mt_100_npt) NPTC = FCO2_ckd_mt_100_npt+1;

  V2C = V1C + FCO2_ckd_mt_100_dv * (Numeric)(NPTC-1);  
  
  if (NPTC < 1)
    {
      out3 << "WARNING:\n"  
           << "  CKD_MT 1.00 CO2 continuum:\n"
           << "  no elements of internal continuum coefficients could be found for the\n"
           << "  input frequency range.\n"
           << "  Leave the function without calculating the absorption.";
      return;
    }

  Numeric FCO2T0[NPTC+addF77fields]; // [cm^3/molecules]

  for (Index J = 1 ; J <= NPTC ; ++J)
    {
      Index I = I1+J;
      if ( (I < 1) || (I > FCO2_ckd_mt_100_npt) ) 
        {
          FCO2T0[J] = 0.0e0;
        }
      else
        {
          FCO2T0[J] = FCO2_ckd_mt_100[I];
        }
    }

  // ---------------------- subroutine FRNCO2 ------------------------------
  
  


  // Loop pressure/temperature:
  for ( Index i = 0 ; i < n_p ; ++i )
    {
      Numeric Tave   = t_abs[i];                               // [K]
      Numeric Pave   = (p_abs[i]*1.000e-2);                    // [hPa]
      // FIXME Numeric vmrco2 = vmr[i];                                 // [1]
      Numeric Rhoave = (Pave/PO) * (TO/Tave);                  // [hPa]
      Numeric WTOT   = xLosmt * (Pave/PO) * (T1/Tave);         // [molecules/cm^2]
      Numeric XKT    = Tave / 1.4387752;                       // = (T*k_B) / (h*c)    
      

      // Molecular cross section calculated by CKD.
      // The cross sectionis calculated on the predefined 
      // CKD wavenumber grid.
      Numeric k[NPTC+addF77fields]; // [1/cm]
      k[0] = 0.00e0; // not used array field
      for (Index J = 1 ; J <= NPTC ; ++J)
        {
          Numeric VJ   = V1C + (DVC * (Numeric)(J-1)); 
          Numeric FCO2 = FCO2T0[J];

          // continuum has been increased in the nu2 band by a factor of 7
          if ( (VJ > 500.0e0) && (VJ < 900.0e0) )
            {
              FCO2 = 7.000e0 * FCO2; 
            }

          // CKD cross section times number density with radiative field [1]
          // the VMRCO2 will be multiplied in absCalc
          k[J] = ((WTOT * Rhoave) * (FCO2*1.000e-20) * RADFN_FUN(VJ,XKT));

        }
      

      // Loop input frequency array. The previously calculated cross section 
      // has therefore to be interpolated on the input frequencies.
      for ( Index s = 0 ; s < n_f ; ++s )
        {
          // calculate the associated wave number (= 1/wavelength)
          Numeric V = f_mono[s] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
          if ( (V > 0.000e0) && (V < FCO2_ckd_mt_100_v2) )
            {
              // arts cross section [1/m]
              // interpolate the k vector on the f_mono grid
              xsec(s,i) +=  ScalingFac * 1.000e2 * XINT_FUN(V1C,V2C,DVC,k,V);
            }
        }
    }
  
}


// =================================================================================
// CKD version MT 1.00 N2-N2 collision induced absorption (rotational band)
// Model reference:
//  Borysow, A, and L. Frommhold, 
//  "Collision-induced rototranslational absorption spectra of N2-N2
//  pairs for temperatures from 50 to 300 K", The
//  Astrophysical Journal, 311, 1043-1057, 1986.
void CKD_mt_CIArot_n2( MatrixView         xsec,
                      const Numeric       Cin,
                      const String&       model,
                      ConstVectorView     f_mono,
                      ConstVectorView     p_abs,
                      ConstVectorView     t_abs,
                      ConstVectorView     vmr )
{

  // check the model name about consistency
  if ((model != "user") &&  (model != "CKDMT100"))
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD_MT1.00 N2 CIA rotational band:\n"
         << "INPUT model name is: " << model << ".\n"
         << "VALID model names are user and CKDMT100\n";
      throw runtime_error(os.str());
    }


  // scaling factor of the N2-N2 CIA rot. band absorption
  Numeric  ScalingFac = 0.0000e0;
  if ( model == "user" )
    {
      ScalingFac = Cin; // input scaling factor of calculated absorption
    }
  else
    {
      ScalingFac = 1.0000e0;
    }

  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies


  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );


  // ************************** CKD stuff ************************************

  // FIXME const Numeric xLosmt = 2.686763e19; // Loschmidt Number [molecules/cm^3]
  const Numeric T1     =  273.0e0;
  const Numeric TO     =  296.0e0;
  const Numeric PO     = 1013.0e0;


  // wavenumber range where CKD H2O self continuum is valid
  const Numeric VABS_min = -1.000e1; // [cm^-1]
  const Numeric VABS_max =  3.500e2; // [cm^-1]


  // It is assumed here that f_mono is monotonically increasing with index!
  // In future change this return into a change of the loop over
  // the frequency f_mono. n_f_new < n_f
  Numeric V1ABS = f_mono[0]     / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  Numeric V2ABS = f_mono[n_f-1] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  if ( (V1ABS < VABS_min) || (V1ABS > VABS_max) ||
       (V2ABS < VABS_min) || (V2ABS > VABS_max) )
    {
      out3  << "WARNING:\n"
            << "  CKD_MT 1.00 N2-N2 CIA rotational band:\n"
            << "  input frequency vector exceeds range of model validity\n"
            << "  " << N2N2_CT296_ckd_mt_100_v1 << "<->" << N2N2_CT220_ckd_mt_100_v2 << "cm^-1\n";
    }


  // ------------------- subroutine N2R296/N2R220 ----------------------------

  if (N2N2_CT296_ckd_mt_100_v1 != N2N2_CT220_ckd_mt_100_v1)
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD_MT 1.00 N2-N2 CIA rotational band:\n"
         << "parameter V1 not the same for different ref. temperatures.\n";
      throw runtime_error(os.str());
    }
  if (N2N2_CT296_ckd_mt_100_v2 != N2N2_CT220_ckd_mt_100_v2)
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD_MT 1.00 N2-N2 CIA rotational band:\n"
         << "parameter V2 not the same for different ref. temperatures.\n";
        throw runtime_error(os.str());
    }
  if (N2N2_CT296_ckd_mt_100_dv != N2N2_CT220_ckd_mt_100_dv)
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD_MT 1.00 N2-N2 CIA rotational band:\n"
         << "parameter DV not the same for different ref. temperatures.\n";
      throw runtime_error(os.str());
    }
  if (N2N2_CT296_ckd_mt_100_npt != N2N2_CT220_ckd_mt_100_npt)
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD_MT 1.00 N2-N2 CIA rotational band:\n"
         << "parameter NPT not the same for different ref. temperatures.\n";
      throw runtime_error(os.str());
    }
  
  // retrieve the appropriate array sequence of the self continuum
  // arrays of the CKD model.
  Numeric DVC = N2N2_CT296_ckd_mt_100_dv;
  Numeric V1C = V1ABS - DVC;
  Numeric V2C = V2ABS + DVC;
  
  int I1 = (int) ((V1C-N2N2_CT296_ckd_mt_100_v1) / N2N2_CT296_ckd_mt_100_dv);
  if (V1C < N2N2_CT296_ckd_mt_100_v1) I1 = -1;
  V1C    = N2N2_CT296_ckd_mt_100_v1 + (N2N2_CT296_ckd_mt_100_dv * (Numeric)I1);

  int I2 = (int) ((V2C-N2N2_CT296_ckd_mt_100_v1) / N2N2_CT296_ckd_mt_100_dv);

  int NPTC = I2-I1+3;
  if (NPTC > N2N2_CT296_ckd_mt_100_npt) NPTC = N2N2_CT296_ckd_mt_100_npt+1;

  V2C    = V1C + N2N2_CT296_ckd_mt_100_dv * (Numeric)(NPTC-1);  
  
  if (NPTC < 1)
    {
      out3 << "WARNING:\n" 
           << "  CKD_MT 1.00 N2-N2 CIA rotational band:\n"
           << "  no elements of internal continuum coefficients could be found for the\n"
           << "  input frequency range.\n"
           << "  Leave the function without calculating the absorption.\n";
      return;
    }

  Numeric C0[NPTC+addF77fields]; // [cm^3/molecules]
  Numeric C1[NPTC+addF77fields]; // [cm^3/molecules]

  for (Index J = 1 ; J <= NPTC ; ++J)
    {
      Index I = I1+J;
      if ( (I < 1) || (I > N2N2_CT296_ckd_mt_100_npt) ) 
        {
          C0[J] = 0.0e0;   // at T=296 K
          C1[J] = 0.0e0;   // at T=260 K
        }
      else
        {
          C0[J] = N2N2_CT296_ckd_mt_100[I];    // at T=296 K
          C1[J] = N2N2_CT220_ckd_mt_100[I];    // at T=260 K 
        }
    }

  // ------------------- subroutine N2R296/N2R220 ----------------------------
  
  


  // Loop pressure/temperature:
  for ( Index i = 0 ; i < n_p ; ++i )
    {
      Numeric Tave   = t_abs[i];                               // [K]
      Numeric Pave   = (p_abs[i]*1.000e-2);                    // [hPa]
      Numeric vmrn2  = vmr[i];                                 // [1]
      Numeric facfac = vmrn2 * (Pave/PO) * (Pave/PO) * 
                               (T1/Tave) * (T1/Tave);

      Numeric XKT    = Tave / 1.4387752;                       // = (T*k_B) / (h*c)    
      Numeric Tfac   = (Tave - TO) / (220.0e0 - TO);

      // Molecular cross section calculated by CKD.
      // The cross sectionis calculated on the predefined 
      // CKD wavenumber grid.
      Numeric k[NPTC+addF77fields]; // [1/cm]
      k[0] = 0.00e0; // not used array field
      for (Index J = 1 ; J <= NPTC ; ++J)
        {
          k[J] = 0.000e0;
          Numeric VJ  = V1C + (DVC * (Numeric)(J-1)); 
          Numeric SN2 = 0.000e0;
          if ( (C0[J] > 0.000e0) && (C1[J] > 0.000e0) )
            {
              SN2 = facfac* C0[J] * pow( (C1[J]/C0[J]), Tfac ); 
            }

          // CKD cross section with radiative field
          k[J] = SN2 * RADFN_FUN(VJ,XKT); // [1]
        }
      

      // Loop input frequency array. The previously calculated cross section 
      // has therefore to be interpolated on the input frequencies.
      for ( Index s = 0 ; s < n_f ; ++s )
        {
          // calculate the associated wave number (= 1/wavelength)
          Numeric V = f_mono[s] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
          if ( (V > 0.000e0) && (V < N2N2_CT220_ckd_mt_100_v2) )
            {
              // arts cross section [1/m]
              // interpolate the k vector on the f_mono grid
              xsec(s,i) +=  ScalingFac * 1.000e2 * XINT_FUN(V1C,V2C,DVC,k,V);
            }
        }
    }
  
}

// =================================================================================

// CKD version MT 1.00 N2-N2 collision induced absorption (fundamental band)
// Model reference:
//  version_1 of the Nitrogen Collision Induced Fundamental
//  Lafferty, W.J., A.M. Solodov,A. Weber, W.B. Olson and 
//  J._M. Hartmann, Infrared collision-induced absorption by 
//  N2 near 4.3 microns for atmospheric applications: 
//  Measurements and emprirical modeling, Appl. Optics, 35, 
//  5911-5917, (1996).
void CKD_mt_CIAfun_n2( MatrixView         xsec,
                      const Numeric       Cin,
                      const String&       model,
                      ConstVectorView     f_mono,
                      ConstVectorView     p_abs,
                      ConstVectorView     t_abs,
                      ConstVectorView     vmr )
{

  // check the model name about consistency
  if ((model != "user") &&  (model != "CKDMT100"))
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD_MT1.00 N2 CIA fundamental band:\n"
         << "INPUT model name is: " << model << ".\n"
         << "VALID model names are user and CKDMT100\n";
      throw runtime_error(os.str());
    }


  // scaling factor of the N2-N2 CIA fundamental band absorption
  Numeric  ScalingFac = 1.0000e0;
  if ( model == "user" )
    {
      ScalingFac = Cin; // input scaling factor of calculated absorption
    }


  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies


  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );


  // ************************** CKD stuff ************************************

  const Numeric xLosmt = 2.686763e19; // Loschmidt Number [molecules/cm^3]
  const Numeric T1     =  273.0e0;
  const Numeric TO     =  296.0e0;
  const Numeric PO     = 1013.0e0;
  const Numeric a1     = 0.8387e0;
  const Numeric a2     = 0.0754e0;


  // It is assumed here that f_mono is monotonically increasing with index!
  // In future change this return into a change of the loop over
  // the frequency f_mono. n_f_new < n_f
  Numeric V1ABS = f_mono[0]     / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  Numeric V2ABS = f_mono[n_f-1] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  if ( (V1ABS < N2N2_N2F_ckd_mt_100_v1) || (V1ABS > N2N2_N2F_ckd_mt_100_v2) ||
       (V2ABS < N2N2_N2F_ckd_mt_100_v1) || (V2ABS > N2N2_N2F_ckd_mt_100_v2) )
    {
      out3  << "WARNING:\n"
            << "   CKD_MT 1.00 N2-N2 CIA fundamental band:\n"
            << "   input frequency vector exceeds range of model validity\n"
            << "  " << N2N2_N2F_ckd_mt_100_v1 << "<->" << N2N2_N2F_ckd_mt_100_v2 << "cm^-1\n";
    }


  // ------------------- subroutine N2_VER_1 ----------------------------
  
  // retrieve the appropriate array sequence of the self continuum
  // arrays of the CKD model.
  Numeric DVC = N2N2_N2F_ckd_mt_100_dv;
  Numeric V1C = V1ABS - DVC;
  Numeric V2C = V2ABS + DVC;
  
  int I1 = (int) ((V1C-N2N2_N2F_ckd_mt_100_v1) / N2N2_N2F_ckd_mt_100_dv);
  if (V1C < N2N2_N2F_ckd_mt_100_v1) I1 = -1;
  V1C    = N2N2_N2F_ckd_mt_100_v1 + (N2N2_N2F_ckd_mt_100_dv * (Numeric)I1);

  int I2 = (int) ((V2C-N2N2_N2F_ckd_mt_100_v1) / N2N2_N2F_ckd_mt_100_dv);

  int NPTC = I2-I1+3;
  if (NPTC > N2N2_N2F_ckd_mt_100_npt) NPTC = N2N2_N2F_ckd_mt_100_npt+1;

  V2C    = V1C + N2N2_N2F_ckd_mt_100_dv * (Numeric)(NPTC-1);  
  
  if (NPTC < 1)
    {
      out3 << "WARNING:\n"  
           << "  CKD_MT 1.00 N2-N2 CIA fundamental band:\n"
           << "  no elements of internal continuum coefficients could be found for the\n"
           << "  input frequency range.\n";
      return;
    }

  Numeric xn2[NPTC+addF77fields];
  Numeric xn2t[NPTC+addF77fields];

  for (Index J = 1 ; J <= NPTC ; ++J)
    {
      xn2[J]  = 0.000e0;
      xn2t[J] = 0.000e0;
      Index I = I1+J;
      if ( (I > 0) && (I <= N2N2_N2F_ckd_mt_100_npt) ) 
        {
          xn2[J]  = N2N2_N2F_ckd_mt_100[I];
          xn2t[J] = N2N2_N2Ft_ckd_mt_100[I];
        }
    }

  // ------------------- subroutine N2_VER_1 ----------------------------
  
  


  // Loop pressure/temperature:
  for ( Index i = 0 ; i < n_p ; ++i )
    {
      Numeric Tave   = t_abs[i];                               // [K]
      Numeric Pave   = (p_abs[i]*1.000e-2);                    // [hPa]
      Numeric vmrn2  = vmr[i];                                 // [1]
      Numeric WTOT   = xLosmt * (Pave/PO) * (T1/Tave);         // [molecules/cm^2]
      Numeric tau_fac= WTOT   * (Pave/PO) * (T1/Tave); 

      Numeric XKT    = Tave / 1.4387752e0;                     // = (T*k_B) / (h*c)    

      // FIXME Numeric Tfac   = (Tave - TO) / (220.0e0 - TO);           // [1]
      Numeric xktfac = (1.000e0/TO) - (1.000e0/Tave);          // [1/K]
      Numeric factor = 0.000e0;
      if (vmrn2 > VMRCalcLimit)
        {
          factor = (1.000e0 / xLosmt) * (1.000e0/vmrn2) * (a1 - a2*(Tave/TO));
        }

      // Molecular cross section calculated by CKD.
      // The cross sectionis calculated on the predefined 
      // CKD wavenumber grid.
      Numeric k[NPTC+addF77fields]; // [1/cm]
      k[0] = 0.000e0; // not used array field
      for (Index J = 1 ; J <= NPTC ; ++J)
        {
          k[J] = 0.000e0;
          Numeric VJ  = V1C + (DVC * (Numeric)(J-1)); 
          Numeric SN2 = 0.000e0;
          if (xn2[J] > 0.000e0)
            {
              Numeric C0 = factor * xn2[J] * exp(xn2t[J]*xktfac) / VJ;
              SN2 = tau_fac * C0;
            }

          // CKD cross section with radiative field
          k[J] = SN2 * RADFN_FUN(VJ,XKT); // [1/cm]
        }
      

      // Loop input frequency array. The previously calculated cross section 
      // has therefore to be interpolated on the input frequencies.
      for ( Index s = 0 ; s < n_f ; ++s )
        {
          // calculate the associated wave number (= 1/wavelength)
          Numeric V = f_mono[s] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
          if ( (V > N2N2_N2F_ckd_mt_100_v1) && (V < N2N2_N2F_ckd_mt_100_v2) )
            {
              // arts cross section [1/m]
              // interpolate the k vector on the f_mono grid
              xsec(s,i) +=  ScalingFac * 1.000e2 * XINT_FUN(V1C,V2C,DVC,k,V);
            }
        }
    }
  
}

// =================================================================================

// CKD version MT 1.00 O2-O2 collision induced absorption (fundamental band)
// Model reference:
// F. Thibault, V. Menoux, R. Le Doucen, L. Rosenman, 
// J.-M. Hartmann, Ch. Boulet, 
// "Infrared collision-induced absorption by O2 near 6.4 microns for
// atmospheric applications: measurements and emprirical modeling", 
// Appl. Optics, 35, 5911-5917, (1996).
void CKD_mt_CIAfun_o2( MatrixView         xsec,
                      const Numeric       Cin,
                      const String&       model,
                      ConstVectorView     f_mono,
                      ConstVectorView     p_abs,
                      ConstVectorView     t_abs,
                      ConstVectorView     vmr )
{

  // check the model name about consistency
  if ((model != "user") &&  (model != "CKDMT100"))
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD_MT1.00 O2 CIA fundamental band:\n"
         << "INPUT model name is: " << model << ".\n"
         << "VALID model names are user and CKDMT100\n";
      throw runtime_error(os.str());
    }


  // scaling factor of the O2-O2 CIA fundamental band absorption
  Numeric  ScalingFac = 1.0000e0;
  if ( model == "user" )
    {
      ScalingFac = Cin; // input scaling factor of calculated absorption
    }


  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies


  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );


  // ************************** CKD stuff ************************************

  const Numeric xLosmt = 2.686763e19; // Loschmidt Number [molecules/cm^3]
  const Numeric T1     =  273.0e0;
  const Numeric TO     =  296.0e0;
  const Numeric PO     = 1013.0e0;


  // It is assumed here that f_mono is monotonically increasing with index!
  // In future change this return into a change of the loop over
  // the frequency f_mono. n_f_new < n_f
  Numeric V1ABS = f_mono[0]     / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  Numeric V2ABS = f_mono[n_f-1] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  if ( (V1ABS < O2O2_O2F_ckd_mt_100_v1) || (V1ABS > O2O2_O2F_ckd_mt_100_v2) ||
       (V2ABS < O2O2_O2F_ckd_mt_100_v1) || (V2ABS > O2O2_O2F_ckd_mt_100_v2) )
    {
      out3  << "WARNING:\n"
            << "  CKD_MT 1.00 O2-O2 CIA fundamental band:\n"
            << "  input frequency vector exceeds range of model validity\n"
            << "  " << O2O2_O2F_ckd_mt_100_v1 << "<->" << O2O2_O2F_ckd_mt_100_v2 << "cm^-1\n";
    }


  // ------------------- subroutine O2_VER_1 ----------------------------
  
  // retrieve the appropriate array sequence of the CKD model array.
  Numeric DVC = O2O2_O2F_ckd_mt_100_dv;
  Numeric V1C = V1ABS - DVC;
  Numeric V2C = V2ABS + DVC;
  
  int I1 = (int) ((V1C-O2O2_O2F_ckd_mt_100_v1) / O2O2_O2F_ckd_mt_100_dv);
  if (V1C < O2O2_O2F_ckd_mt_100_v1) I1 = -1;
  V1C    = O2O2_O2F_ckd_mt_100_v1 + (O2O2_O2F_ckd_mt_100_dv * (Numeric)I1);

  int I2 = (int) ((V2C-O2O2_O2F_ckd_mt_100_v1) / O2O2_O2F_ckd_mt_100_dv);

  int NPTC = I2-I1+3;
  if (NPTC > O2O2_O2F_ckd_mt_100_npt) NPTC = O2O2_O2F_ckd_mt_100_npt+1;

  V2C    = V1C + O2O2_O2F_ckd_mt_100_dv * (Numeric)(NPTC-1);  
  
  if (NPTC < 1)
    {
      out3 << "WARNING:\n"
           << "  CKD_MT 1.00 O2 CIA fundamental band:\n"
           << "  no elements of internal continuum coefficients could be found for the\n"
           << "  input frequency range.\n"
           << "  Leave the function without calculating the absorption.\n";
      return;
    }

  Numeric xo2[NPTC+addF77fields];
  Numeric xo2t[NPTC+addF77fields];

  for (Index J = 1 ; J <= NPTC ; ++J)
    {
      xo2[J]  = 0.000e0;
      xo2t[J] = 0.000e0;
      Index I = I1+J;
      if ( (I > 0) && (I <= O2O2_O2F_ckd_mt_100_npt) ) 
        {
          xo2[J]  = O2O2_O2Fo_ckd_mt_100[I];
          xo2t[J] = O2O2_O2Ft_ckd_mt_100[I];
        }
    }

  // ------------------- subroutine O2_VER_1 ----------------------------
  
  


  // Loop pressure/temperature:
  for ( Index i = 0 ; i < n_p ; ++i )
    {
      Numeric Tave   = t_abs[i];                               // [K]
      Numeric Pave   = (p_abs[i]*1.000e-2);                    // [hPa]
      // FIXME Numeric vmro2  = vmr[i];                                 // [1]
      Numeric WTOT   = xLosmt * (Pave/PO) * (T1/Tave);         // [molecules/cm^2]
      Numeric tau_fac= WTOT * (Pave/PO) * (T1/Tave);

      Numeric XKT    = Tave / 1.4387752;                       // = (T*k_B) / (h*c)    

      Numeric xktfac = (1.000e0/TO) - (1.000e0/Tave);          // [1/K]
      Numeric factor = (1.000e0 / xLosmt);

      // Molecular cross section calculated by CKD.
      // The cross sectionis calculated on the predefined 
      // CKD wavenumber grid.
      Numeric k[NPTC+addF77fields]; // [1/cm]
      k[0] = 0.00e0; // not used array field
      for (Index J = 1 ; J <= NPTC ; ++J)
        {
          Numeric VJ  = V1C + (DVC * (Numeric)(J-1)); 
          Numeric SO2 = 0.0e0;
          if (xo2[J] > 0.0e0)
            {
              Numeric C0 = factor * xo2[J] * exp(xo2t[J]*xktfac) / VJ;
              SO2 = tau_fac * C0;
            }

          // CKD cross section without radiative field
          k[J] = SO2 * RADFN_FUN(VJ,XKT); // [1]
        }
      

      // Loop input frequency array. The previously calculated cross section 
      // has therefore to be interpolated on the input frequencies.
      for ( Index s = 0 ; s < n_f ; ++s )
        {
          // calculate the associated wave number (= 1/wavelength)
          Numeric V = f_mono[s] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
          if ( (V > O2O2_O2F_ckd_mt_100_v1) && (V < O2O2_O2F_ckd_mt_100_v2) )
            {
              // arts cross section [1/m]
              // interpolate the k vector on the f_mono grid
              xsec(s,i) +=  ScalingFac * 1.000e2 * XINT_FUN(V1C,V2C,DVC,k,V);
            }
        }
    }
  
}

// =================================================================================

// CKD version MT 1.00 O2 v0<-v0 band absorption
// Model reference:
// CKD_MT 1.00 implementation of oxygen collision induced fundamental model of 
// O2 continuum formulated by 
//   Mate et al. over the spectral region 7550-8486 cm-1: 
//   B. Mate, C. Lugez, G.T. Fraser, W.J. Lafferty,
//   "Absolute Intensities for the O2 1.27 micron
//   continuum absorption",  
//   J. Geophys. Res., 104, 30,585-30,590, 1999. 
//
// The units of these continua coefficients are  1 / (amagat_O2*amagat_air)
//
// Also, refer to the paper "Observed  Atmospheric
// Collision Induced Absorption in Near Infrared Oxygen Bands",
// Mlawer, Clough, Brown, Stephen, Landry, Goldman, & Murcray,
// Journal of Geophysical Research (1997).
void CKD_mt_v0v0_o2( MatrixView          xsec,
                     const Numeric       Cin,
                     const String&       model,
                     ConstVectorView     f_mono,
                     ConstVectorView     p_abs,
                     ConstVectorView     t_abs,
                     ConstVectorView     vmr,
                     ConstVectorView     n2_abs)
{


  // check the model name about consistency
  if ((model != "user") &&  (model != "CKDMT100"))
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD_MT1.00 O2 band at 1.27 micrometer:\n"
         << "INPUT model name is: " << model << ".\n"
         << "VALID model names are user and CKDMT100\n";
      throw runtime_error(os.str());
    }


  // scaling factor of the O2 v0<-v0 band absorption
  Numeric  ScalingFac = 1.0000e0;
  if ( model == "user" )
    {
      ScalingFac = Cin; // input scaling factor of calculated absorption
    };

  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies


  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );


  // ************************** CKD stuff ************************************

  // FIXME const Numeric xLosmt    = 2.686763e19; // Loschmidt Number [molecules/cm^3]
  const Numeric T1        =  273.0e0;
  // FIXME const Numeric TO        =  296.0e0;
  const Numeric PO        = 1013.0e0;

  // It is assumed here that f_mono is monotonically increasing with index!
  // In future change this return into a change of the loop over
  // the frequency f_mono. n_f_new < n_f
  Numeric V1ABS = f_mono[0]     / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  Numeric V2ABS = f_mono[n_f-1] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  if ( (V1ABS < O2_00_ckd_mt_100_v1) || (V1ABS > O2_00_ckd_mt_100_v2) ||
       (V2ABS < O2_00_ckd_mt_100_v1) || (V2ABS > O2_00_ckd_mt_100_v2) )
    {
      out3  << "WARNING:\n"
            << "   CKD_MT 1.00 O2 v0<-v0 band:\n"
            << "   input frequency vector exceeds range of model validity\n"
            << "  " << O2_00_ckd_mt_100_v1 << "<->" << O2_00_ckd_mt_100_v2 << "cm^-1\n";
    }


  // ------------------- subroutine O2INF1 ----------------------------
  
  // retrieve the appropriate array sequence of the CKD model array.
  Numeric DVC = O2_00_ckd_mt_100_dv;
  Numeric V1C = V1ABS - DVC;
  Numeric V2C = V2ABS + DVC;
  
  int I1 = (int) ((V1C-O2_00_ckd_mt_100_v1) / O2_00_ckd_mt_100_dv);
  if (V1C < O2_00_ckd_mt_100_v1) I1 = I1-1;
  V1C    = O2_00_ckd_mt_100_v1 + (O2_00_ckd_mt_100_dv * (Numeric)I1);

  int I2 = (int) ((V2C-O2_00_ckd_mt_100_v1) / O2_00_ckd_mt_100_dv);

  int NPTC = I2-I1+3;

  V2C    = V1C + O2_00_ckd_mt_100_dv * (Numeric)(NPTC-1);  
  
  if (NPTC < 1)
    {
      out3 << "WARNING:\n"  
           << "  CKD_MT 1.00 O2 v0<-v0 band:\n"
           << "  no elements of internal continuum coefficients could be found for the\n"
           << "  input frequency range.\n"
           << "  Leave the function without calculating the absorption.\n";
      return;
    }

  Numeric CO[(int)(NPTC+addF77fields)];


  for (Index J = 1 ; J <= NPTC ; ++J)
    {
      CO[J]  = 0.000e0;
      Index I = I1+J;
      if ( (I > 0) && (I <= O2_00_ckd_mt_100_npt) ) 
        {
          Numeric VJ  = V1C + (DVC * (Numeric)(J-1)); 
          CO[J]  = O2_00_ckd_mt_100[I] / VJ;
        }
    }

  // ------------------- subroutine O2INF1 ----------------------------
  
  


  // Loop pressure/temperature:
  for ( Index i = 0 ; i < n_p ; ++i )
    {
      Numeric Tave   = t_abs[i];                               // [K]
      Numeric Pave   = (p_abs[i]*1.000e-2);                    // [hPa]
      Numeric vmro2  = vmr[i];                                 // [1]
      Numeric vmrn2  = n2_abs[i];                              // [1]
      Numeric ADJWO2 = (vmro2 + 0.300e0*vmrn2) / 0.446e0 * 
                       (Pave/PO) * (Pave/PO) * (T1/Tave) * (T1/Tave);
      Numeric XKT    = Tave / 1.4387752e0;                     // = (T*k_B) / (h*c)    

      // Molecular cross section calculated by CKD.
      // The cross sectionis calculated on the predefined 
      // CKD wavenumber grid. The abs. coeff. is then the 
      // cross section times the number density.
      Numeric k[NPTC+addF77fields]; // [1/cm]
      k[0] = 0.00e0; // not used array field
      for (Index J = 1 ; J <= NPTC ; ++J)
        {
          Numeric VJ  = V1C + (DVC * (Numeric)(J-1)); 
          Numeric SO2 = 0.0e0;
          if (CO[J] > 0.0e0)
            {
              SO2 = ADJWO2 * CO[J];
            }

          // CKD (cross section * number density) with radiative field
          k[J] = SO2 * RADFN_FUN(VJ,XKT); // [1/cm]
        }
      

      // Loop input frequency array. The previously calculated cross section 
      // has therefore to be interpolated on the input frequencies.
      for ( Index s = 0 ; s < n_f ; ++s )
        {
          // calculate the associated wave number (= 1/wavelength)
          Numeric V = f_mono[s] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
          if ( (V > O2_00_ckd_mt_100_v1) && (V < O2_00_ckd_mt_100_v2) )
            {
              // arts cross section [1/m]
              // interpolate the k vector on the f_mono grid
              xsec(s,i) +=  ScalingFac * 1.000e2 * XINT_FUN(V1C,V2C,DVC,k,V);
            }
        }
    }
  
}

// =================================================================================

// CKD version MT 1.00 O2 v1<-v0 band absorption
// Model reference:
// CKD_MT 1.00 implementation of oxygen v1<-v0 band model of 
// Mlawer, Clough, Brown, Stephen, Landry, Goldman, Murcray,
// "Observed  Atmospheric Collision Induced Absorption in Near Infrared Oxygen Bands",
// Journal of Geophysical Research, vol 103, no. D4, pp. 3859-3863, 1998.
void CKD_mt_v1v0_o2( MatrixView          xsec,
                     const Numeric       Cin,
                     const String&       model,
                     ConstVectorView     f_mono,
                     ConstVectorView     p_abs,
                     ConstVectorView     t_abs,
                     ConstVectorView     vmr )
{

  // check the model name about consistency
  if ((model != "user") &&  (model != "CKDMT100"))
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKD_MT1.00 O2 band at 1.06 micrometer:\n"
         << "INPUT model name is: " << model << ".\n"
         << "VALID model names are user and CKDMT100\n";
      throw runtime_error(os.str());
    }


  // scaling factor of the O2 v1<-v0 band absorption
  Numeric  ScalingFac = 1.0000e0;
  if ( model == "user" )
    {
      ScalingFac = Cin; // input scaling factor of calculated absorption
    };

  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies


  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );


  // ************************** CKD stuff ************************************

  const Numeric xLosmt    = 2.686763e19; // Loschmidt Number [molecules/cm^3]
  const Numeric T1        =  273.0e0;
  const Numeric TO        =  296.0e0;
  const Numeric PO        = 1013.0e0;
  // FIXME const Numeric vmr_argon = 9.000e-3;    // VMR of argon is assumed to be const.


  // CKD_MT 1.00 implementation of oxygen v1<-v0 band model of
  // Mlawer, Clough, Brown, Stephen, Landry, Goldman, Murcray,
  // "Observed  Atmospheric Collision Induced Absorption in Near Infrared Oxygen Bands",
  // Journal of Geophysical Research, vol 103, no. D4, pp. 3859-3863, 1998.
  const Numeric V1S    = O2_10_ckd_mt_100_v1;
  const Numeric V2S    = O2_10_ckd_mt_100_v2;
  const Numeric DVS    = O2_10_ckd_mt_100_dv;
  const Numeric V1_osc =  9375.000e0;
  const Numeric HW1    =    58.960e0;
  const Numeric V2_osc =  9439.000e0;
  const Numeric HW2    =    45.040e0;
  const Numeric S1     =     1.166e-4;
  const Numeric S2     =     3.086e-5;


  // It is assumed here that f_mono is monotonically increasing with index!
  // In future change this return into a change of the loop over
  // the frequency f_mono. n_f_new < n_f
  Numeric V1ABS = f_mono[0]     / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  Numeric V2ABS = f_mono[n_f-1] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
  if ( (V1ABS < O2_10_ckd_mt_100_v1) || (V1ABS > O2_10_ckd_mt_100_v2) ||
       (V2ABS < O2_10_ckd_mt_100_v1) || (V2ABS > O2_10_ckd_mt_100_v2) )
    {
      out3  << "WARNING:\n"
            << "   CKD_MT 1.00 O2 v1<-v0 band:\n"
            << "   input frequency vector exceeds range of model validity\n"
            << "  " << O2_10_ckd_mt_100_v1 << "<->" << O2_10_ckd_mt_100_v2 << "cm^-1\n";
    }


  // ------------------- subroutine O2INF2 ----------------------------
  
  // retrieve the appropriate array sequence of the CKD model array.
  Numeric DVC = DVS;
  Numeric V1C = V1ABS - DVC;
  Numeric V2C = V2ABS + DVC;
  
  int NPTC = (int)( ((V2C-V1C)/DVC) + 3 );

  V2C = V1C + ( DVC * (Numeric)(NPTC-1) );
  
  if (NPTC < 1)
    {
      out3 << "WARNING:\n" 
           << "  CKD_MT 1.00 O2 v1<-v0 band:\n"
           << "  no elements of internal continuum coefficients could be found for the\n"
           << "  input frequency range.\n"
           << "  Leave the function without calculating the absorption.\n";
      return;
    }

  Numeric C[NPTC+addF77fields];
  C[0] = 0.000e0; // not used field of array

  for (Index J = 1 ; J <= NPTC ; ++J)
    {
      C[J]  = 0.000e0;
      Numeric VJ  = V1C + (DVC * (Numeric)(J-1)); 

      if ( (VJ > V1S) && (VJ < V2S) ) 
        {
          Numeric DV1 = VJ - V1_osc;
          Numeric DV2 = VJ - V2_osc;

          Numeric DAMP1 = 1.00e0;
          Numeric DAMP2 = 1.00e0;

          if ( DV1 < 0.00e0 ) 
            {
              DAMP1 = exp(DV1 / 176.100e0);
            }

          if ( DV2 < 0.00e0 ) 
            {
              DAMP2 = exp(DV2 / 176.100e0);
            }
          
          Numeric O2INF = 0.31831e0 * 
                 ( ((S1 * DAMP1 / HW1)/(1.000e0 + pow((DV1/HW1),(Numeric)2.0e0) )) + 
                   ((S2 * DAMP2 / HW2)/(1.000e0 + pow((DV2/HW2),(Numeric)2.0e0) )) ) * 1.054e0;
          C[J] = O2INF / VJ;
        }
    }


  // ------------------- subroutine O2INF2 ----------------------------
  
  
  // Loop pressure/temperature:
  for ( Index i = 0 ; i < n_p ; ++i )
    {
      Numeric Tave   = t_abs[i];                               // [K]
      Numeric Pave   = (p_abs[i]*1.000e-2);                    // [hPa]
      Numeric vmro2  = vmr[i];                                 // [1]
      Numeric WTOT   = 1.000e-20 * xLosmt * (Pave/PO) * (T1/Tave); // [molecules/cm^2]
      Numeric ADJWO2 = (vmro2 / 0.209e0) * WTOT * (Pave/PO) * (TO/Tave);
      Numeric XKT    = Tave / 1.4387752;                       // = (T*k_B) / (h*c)    

      // Molecular cross section calculated by CKD.
      // The cross sectionis calculated on the predefined 
      // CKD wavenumber grid.
      Numeric k[NPTC+addF77fields]; // [1/cm]
      k[0] = 0.00e0; // not used array field
      for (Index J = 1 ; J <= NPTC ; ++J)
        {
          Numeric VJ  = V1C + (DVC * (Numeric)(J-1)); 
          Numeric SO2 = 0.0e0;
          if (C[J] > 0.0e0)
            {
              SO2 = ADJWO2 * C[J];
            }

          // CKD cross section without radiative field
          k[J] = SO2 * RADFN_FUN(VJ,XKT); // [1]
        }
      

      // Loop input frequency array. The previously calculated cross section 
      // has therefore to be interpolated on the input frequencies.
      for ( Index s = 0 ; s < n_f ; ++s )
        {
          // calculate the associated wave number (= 1/wavelength)
          Numeric V = f_mono[s] / (SPEED_OF_LIGHT * 1.00e2); // [cm^-1]
          if ( (V > V1S) && (V < V2S) )
            {
              // arts cross section [1/m]
              // interpolate the k vector on the f_mono grid
              xsec(s,i) +=  ScalingFac * 1.000e2 * XINT_FUN(V1C,V2C,DVC,k,V);
            }
        }
    }
  
}

// #################################################################################

// CKD version 2.4 H2O continuum absorption model
void CKD24_H20( MatrixView          xsec,
                int                 isf,
                const Numeric       Cin,
                const String&       model,
                ConstVectorView     f_mono,
                ConstVectorView     p_abs,
                ConstVectorView     t_abs,
                ConstVectorView     vmr,
                ConstVectorView     n2_abs )
{
  //
  //
  // external function to call (original F77 code translated with f2c)
  /* INPUT PARAMETERS:                           */
  /*  P          [hPa]  TOTAL PRESSURE           */
  /*  T          [K]    TEMPERATURE              */
  /*  VMRH2O     [1]    H2O VOLUME MIXING RATIO  */
  /*  VMRN2      [1]    N2  VOLUME MIXING RATIO  */
  /*  VMRO2      [1]    O2  VOLUME MIXING RATIO  */
  /*  FREQ       [Hz]   FREQUENCY OF CALCULATION */
  extern double artsckd_(double p, double t, 
                         double vmrh2o, double vmrn2, double vmro2, 
                         double freq, int ivc);
  //
  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  Numeric  XFAC  =  1.0000;             // scaling factor
  // ---------------------------------------------------------------------------------------
  

  // check the model name about consistency
  if ((model != "user") &&  (model != "CKD24"))
    {
      ostringstream os;
      os << "!!ERROR!!\n"  
         << "CKDv2.4.2 H2O self/foreign continuum:\n"
         << "INPUT model name is: " << model << ".\n"
         << "VALID model names are user and CKD24\n";
      throw runtime_error(os.str());
    }


  // select the parameter set (!!model dominates values!!):
  if ( model == "CKD24" )
    {
      XFAC =  1.0000;
    }
  else if ( model == "user" )
    {
      XFAC =  Cin;
    }
  else
    {
      if (isf == 0) {
        ostringstream os;
        os << "H2O-SelfContCKD24: ERROR! Wrong model values given.\n"
           << "allowed models are: 'CKD24', 'user'" << '\n';
        throw runtime_error(os.str());
      }
      if (isf == 1) {
        ostringstream os;
        os << "H2O-ForeignContCKD: ERROR! Wrong model values given.\n"
           << "allowed models are: 'CKD24', 'user'" << '\n';
        throw runtime_error(os.str());
      }
    }
  
  if (isf == 0) {
    out3  << "H2O-SelfContCKD24: (model=" << model << ") parameter values in use:\n" 
          << " XFAC = " << XFAC << "\n";
  }
  if (isf == 1) {
    out3  << "H2O-ForeignContCKD: (model=" << model << ") parameter values in use:\n" 
          << " XFAC = " << XFAC << "\n";
  }


  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies


  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );
  
  //  ivc = 1     : N2-N2 CKD version of Borysow-Fromhold model
  //  ivc = 21    : H2O CKD2.4  self cont part
  //  ivc = 22    : H2O CKD2.4  foreign cont part 
  //  ivc = 31    : MPMf87/s93  self cont part
  //  ivc = 32    : MPMf87/s93  foreign cont part 
  int ivc = 55;
  if (isf == 0) {
    ivc = 21; // CKD2.4  self continuum
    // ivc = 31; // MPMf87/s93  self continuum
  }
  if (isf == 1) {
    ivc = 22; // CKD2.4  foreign continuum
    //ivc = 32; // MPMf87/s93  foreign continuum
  }
  if ((ivc != 1) && (ivc != 21) && (ivc != 22) && (ivc != 31) && (ivc != 32)) {
    ostringstream os;
    os << "!!ERROR: CKD24 H2O model: wrong input parameter isf (=0,1) given!\n"
       << "retrun without calculation!" << "\n"
       << "actual value of isf is " << isf << "\n";
    throw runtime_error(os.str());
    return;
  }
  // ivc = 1;

  // Loop pressure/temperature:
  for ( Index i=0; i<n_p; ++i )
    {
      double T      = (double) t_abs[i];            // [K]
      double p      = (double) (p_abs[i]*1.000e-2); // [hPa]
      double vmrh2o = (double) vmr[i];              // [1]
      double vmrn2  = (double) n2_abs[i];           // [1]
      double vmro2  = 0.0e0;                        // [1]

      //cout << "------------------------------------------------\n";
      //cout << "CKD2.4 H2O: ivc   =" << ivc << "\n";
      //cout << "CKD2.4 H2O: T     =" << T << " K\n";
      //cout << "CKD2.4 H2O: p     =" << p << " hPa\n";
      //cout << "CKD2.4 H2O: vmrh2o=" << vmrh2o << "\n";
      //cout << "CKD2.4 H2O: vmrn2 =" << vmrn2 << "\n";
      //cout << "CKD2.4 H2O: vmro2 =" << vmro2 << "\n";
      // Loop frequency:
      for ( Index s=0; s<n_f; ++s )
        {
          // the second vmr of N2 will be multiplied at the stage of
          // absorption calculation: abs =  vmr * xsec.
          double f = (double) f_mono[s];            // [Hz]
          if (ivc == 1) { // ---------- N2 -----------------
            if (n2_abs[i] > 0.0e0) {
              //cout << "CKD2.4 N2: f   =" << f << " Hz\n";
              double cont = artsckd_(p, T, vmrh2o, vmrn2, vmro2, f, ivc);
              xsec(s,i) +=  (Numeric) (cont / vmr[i]);
              //cout << "CKD2.4 N2: abs =" << cont << " 1/m\n";
            }
          } else { // ---------------- H2O -----------------
            if (vmr[i] > 0.0e0) {
              //cout << "CKD2.4 H2O: f   =" << f << " Hz\n";
              double cont = artsckd_(p, T, vmrh2o, vmrn2, vmro2, f, ivc);
              xsec(s,i) +=  (Numeric) (cont / vmr[i]);
              //cout << "CKD2.4 H2O: abs =" << cont << " 1/m\n";
            }
          }
        }
    }
  return;
}
//
// #################################################################################
//
void Pardo_ATM_H2O_ForeignContinuum( MatrixView          xsec,
                                     const Numeric       Cin,
                                     const String&       model,
                                     ConstVectorView     f_mono,
                                     ConstVectorView     p_abs,
                                     ConstVectorView     t_abs,
                                     ConstVectorView     vmr)
{
  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the Pardo et al. model (IEEE, Trans. Ant. Prop., 
  // Vol 49, No 12, pp. 1683-1694, 2001)
  const Numeric C_ATM = 0.0315; // [1/m]
  // ---------------------------------------------------------------------------------------

  // select the parameter set (!!model dominates parameters!!):
  Numeric C;
   if ( model == "ATM" )
     {
       C = C_ATM;
     }
   else if ( model == "user" )
     {
       C = Cin;
     }
   else
     {
       ostringstream os;
       os << "H2O-ForeignContATM01: ERROR! Wrong model values given.\n"
          << "allowed models are: 'ATM', 'user'" << '\n';
       throw runtime_error(os.str());
     }
   out3  << "H2O-ForeignContATM01: (model=" << model << ") parameter values in use:\n" 
         << " C_f = " << C << "\n";

   const Index n_p = p_abs.nelem();     // Number of pressure levels
   const Index n_f = f_mono.nelem();    // Number of frequencies

   // Check that dimensions of p_abs, t_abs, and vmr agree:
   assert ( n_p==t_abs.nelem() );
   assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );
  
  // Loop over pressure/temperature grid:
  for ( Index i=0; i<n_p; ++i )
    {
      // since this is an effective "dry air" continuum, it is not really
      // it is not specifically attributed to N2, so we need the total 
      // dry air part in total which is equal to the total minus the 
      // water vapor pressure:
      Numeric  pd = p_abs[i] * ( 1.00000e0 - vmr[i] ); // [Pa]
      // since the H2O VMR will be multiplied in absCalc, we omit it here
      Numeric  pwdummy = p_abs[i]                    ; // [Pa]
      // Loop over frequency grid:
      for ( Index s=0; s<n_f; ++s )
        {
          // Becaue this is an effective "dry air" continuum, it is not really
          // specific N2 but mainly caused by N2. Therefore the N2 vmr must be 
          // canceled out here which is later in absCalc multiplied 
          // (calculation: abs = vmr * xsec):
          xsec(s,i) += C *                  // strength [1/(m*Hz²Pa²)] 
            pow( (f_mono[s]/(Numeric)2.25e11), (Numeric)2. ) * // quadratic f dependence [1]
            pow( ((Numeric)300.0/t_abs[i]), (Numeric)3. ) * // free T dependence      [1]
            (pd/1.01300e5)                * // p_dry dependence       [1]
            (pwdummy/1.01300e5);            // p_H2O dependence       [1]
        }
    }
}
//
// #################################################################################
//
// MPM93 H2O pseudo continuum line parameters:
// see publication side of National Telecommunications and Information Administration
//   http://www.its.bldrdoc.gov/pub/all_pubs/all_pubs.html
// and ftp side for downloading the MPM93 original source code:
//   ftp://ftp.its.bldrdoc.gov/pub/mpm93/
void MPM93_H2O_continuum( MatrixView          xsec,
                          const Numeric       fcenter,
                          const Numeric       b1,
                          const Numeric       b2,
                          const Numeric       b3,
                          const Numeric       b4,
                          const Numeric       b5,
                          const Numeric       b6,
                          const String&       model,
                          ConstVectorView     f_mono,
                          ConstVectorView     p_abs,
                          ConstVectorView     t_abs,
                          ConstVectorView     vmr        )
{

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the MPM93 H2O continuum model 
  // (AGARD 52nd Specialists Meeting of the Electromagnetic Wave
  // Propagation Panel, Palma de Mallorca, Spain, 1993, May 17-21):
  const Numeric MPM93fo_orig =  1780.000e9;  // [Hz]
  const Numeric MPM93b1_orig = 22300.000;    // [Hz/Pa]
  const Numeric MPM93b2_orig =     0.952;    // [1]
  const Numeric MPM93b3_orig =    17.600e4;  // [Hz/Pa]
  const Numeric MPM93b4_orig =    30.500;    // [1]
  const Numeric MPM93b5_orig =     2.000;    // [1]
  const Numeric MPM93b6_orig =     5.000;    // [1]
  // ---------------------------------------------------------------------------------------
  

  // select the parameter set (!!model goes for values!!):
  Numeric MPM93fopcl, MPM93b1pcl, MPM93b2pcl, 
          MPM93b3pcl, MPM93b4pcl, MPM93b5pcl,
          MPM93b6pcl;
  if ( model == "MPM93" )
    {
      MPM93fopcl =  MPM93fo_orig;
      MPM93b1pcl =  MPM93b1_orig;
      MPM93b2pcl =  MPM93b2_orig;
      MPM93b3pcl =  MPM93b3_orig;
      MPM93b4pcl =  MPM93b4_orig;
      MPM93b5pcl =  MPM93b5_orig;
      MPM93b6pcl =  MPM93b6_orig;
    }
  else if ( model == "user" )
     {
      MPM93fopcl =  fcenter;
      MPM93b1pcl =  b1;
      MPM93b2pcl =  b2;
      MPM93b3pcl =  b3;
      MPM93b4pcl =  b4;
      MPM93b5pcl =  b5;
      MPM93b6pcl =  b6;
    }
   else
     {
       ostringstream os;
       os << "H2O-ContMPM93: ERROR! Wrong model values given.\n"
          << "allowed models are: 'MPM93', 'user'" << '\n';
       throw runtime_error(os.str());
     }
   out3  << "H2O-ContMPM93: (model=" << model << ") parameter values in use:\n" 
         << " fo = " << MPM93fopcl << "\n"
         << " b1 = " << MPM93b1pcl << "\n"
         << " b2 = " << MPM93b2pcl << "\n"
         << " b3 = " << MPM93b3pcl << "\n"
         << " b4 = " << MPM93b4pcl << "\n"
         << " b5 = " << MPM93b5pcl << "\n"
         << " b6 = " << MPM93b6pcl << "\n";

  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );
  

  // Loop pressure/temperature:
  for ( Index i=0; i<n_p; ++i )
    {
      Numeric th = 300.0 / t_abs[i];
      // the vmr of H2O will be multiplied at the stage of absorption calculation:
      // abs / vmr * xsec.
      Numeric strength =  MPM93b1pcl * p_abs[i] * pow( th, (Numeric)3.5 )
        * exp(MPM93b2pcl * (1 - th));
      Numeric gam      =  MPM93b3pcl * 0.001 * 
                          ( MPM93b4pcl * p_abs[i] * vmr[i]       * pow( th, MPM93b6pcl ) +  
                                         p_abs[i]*(1.000-vmr[i]) * pow( th, MPM93b5pcl ) );
      // Loop frequency:
      for ( Index s=0; s<n_f; ++s )
        {
          // xsec = abs/vmr [1/m] but MPM89 is in [dB/km] --> conversion necessary
          xsec(s,i) += dB_km_to_1_m * 0.1820 *
                       f_mono[s] * strength * 
                       MPMLineShapeFunction(gam, MPM93fopcl, f_mono[s]); 
        }
    }
  return;
}
//
// #################################################################################
// ################################# OXYGEN MODELS #################################
// #################################################################################
void MPM85O2AbsModel( MatrixView          xsec,
                      const Numeric       CCin,       // continuum scale factor 
                      const Numeric       CLin,       // line strength scale factor
                      const Numeric       CWin,       // line broadening scale factor
                      const Numeric       COin,       // line coupling scale factor
                      const String&       model,
                      ConstVectorView     f_mono,
                      ConstVectorView     p_abs,
                      ConstVectorView     t_abs,
                      ConstVectorView     h2o_abs,
                      ConstVectorView     vmr )
{
  //
  // Coefficients are from Liebe et al., AGARD CP-May93, Paper 3/1-10
  //      0             1           2         3          4      5         6
  //      f0           a1          a2        a3         a4     a5        a6
  //    [GHz]      [kHz/hPa]      [1]     [MHz/hPa]    [1]   [1/kPa]     [1]
  const Numeric mpm85[48][7] = { 
   { 49.452379 ,       0.12 ,    11.830 ,    8.40 ,    0.0 ,  5.600 ,   1.700 },
   { 49.962257 ,       0.34 ,    10.720 ,    8.50 ,    0.0 ,  5.600 ,   1.700 },
   { 50.474238 ,       0.94 ,     9.690 ,    8.60 ,    0.0 ,  5.600 ,   1.700 },
   { 50.987748 ,       2.46 ,     8.690 ,    8.70 ,    0.0 ,  5.500 ,   1.700 },
   { 51.503350 ,       6.08 ,     7.740 ,    8.90 ,    0.0 ,  5.600 ,   1.800 },
   { 52.021409 ,      14.14 ,     6.840 ,    9.20 ,    0.0 ,  5.500 ,   1.800 },
   { 52.542393 ,      31.02 ,     6.000 ,    9.40 ,    0.0 ,  5.700 ,   1.800 },
   { 53.066906 ,      64.10 ,     5.220 ,    9.70 ,    0.0 ,  5.300 ,   1.900 },
   { 53.595748 ,     124.70 ,     4.480 ,   10.00 ,    0.0 ,  5.400 ,   1.800 },
   { 54.129999 ,     228.00 ,     3.810 ,   10.20 ,    0.0 ,  4.800 ,   2.000 },
   { 54.671157 ,     391.80 ,     3.190 ,   10.50 ,    0.0 ,  4.800 ,   1.900 },
   { 55.221365 ,     631.60 ,     2.620 ,   10.79 ,    0.0 ,  4.170 ,   2.100 },
   { 55.783800 ,     953.50 ,     2.115 ,   11.10 ,    0.0 ,  3.750 ,   2.100 },
   { 56.264777 ,     548.90 ,     0.010 ,   16.46 ,    0.0 ,  7.740 ,   0.900 },
   { 56.363387 ,    1344.00 ,     1.655 ,   11.44 ,    0.0 ,  2.970 ,   2.300 },
   { 56.968180 ,    1763.00 ,     1.255 ,   11.81 ,    0.0 ,  2.120 ,   2.500 },
   { 57.612481 ,    2141.00 ,     0.910 ,   12.21 ,    0.0 ,  0.940 ,   3.700 },
   { 58.323874 ,    2386.00 ,     0.621 ,   12.66 ,    0.0 , -0.550 ,  -3.100 },
   { 58.446589 ,    1457.00 ,     0.079 ,   14.49 ,    0.0 ,  5.970 ,   0.800 },
   { 59.164204 ,    2404.00 ,     0.386 ,   13.19 ,    0.0 , -2.440 ,   0.100 },
   { 59.590982 ,    2112.00 ,     0.207 ,   13.60 ,    0.0 ,  3.440 ,   0.500 },
   { 60.306057 ,    2124.00 ,     0.207 ,   13.82 ,    0.0 , -4.130 ,   0.700 },
   { 60.434775 ,    2461.00 ,     0.386 ,   12.97 ,    0.0 ,  1.320 ,  -1.000 },
   { 61.150558 ,    2504.00 ,     0.621 ,   12.48 ,    0.0 , -0.360 ,   5.800 },
   { 61.800152 ,    2298.00 ,     0.910 ,   12.07 ,    0.0 , -1.590 ,   2.900 },
   { 62.411212 ,    1933.00 ,     1.255 ,   11.71 ,    0.0 , -2.660 ,   2.300 },
   { 62.486253 ,    1517.00 ,     0.078 ,   14.68 ,    0.0 , -4.770 ,   0.900 },
   { 62.997974 ,    1503.00 ,     1.660 ,   11.39 ,    0.0 , -3.340 ,   2.200 },
   { 63.568515 ,    1087.00 ,     2.110 ,   11.08 ,    0.0 , -4.170 ,   2.000 },
   { 64.127764 ,     733.50 ,     2.620 ,   10.78 ,    0.0 , -4.480 ,   2.000 },
   { 64.678900 ,     463.50 ,     3.190 ,   10.50 ,    0.0 , -5.100 ,   1.800 },
   { 65.224067 ,     274.80 ,     3.810 ,   10.20 ,    0.0 , -5.100 ,   1.900 },
   { 65.764769 ,     153.00 ,     4.480 ,   10.00 ,    0.0 , -5.700 ,   1.800 },
   { 66.302088 ,      80.09 ,     5.220 ,    9.70 ,    0.0 , -5.500 ,   1.800 },
   { 66.836827 ,      39.46 ,     6.000 ,    9.40 ,    0.0 , -5.900 ,   1.700 },
   { 67.369595 ,      18.32 ,     6.840 ,    9.20 ,    0.0 , -5.600 ,   1.800 },
   { 67.900862 ,       8.01 ,     7.740 ,    8.90 ,    0.0 , -5.800 ,   1.700 },
   { 68.431001 ,       3.30 ,     8.690 ,    8.70 ,    0.0 , -5.700 ,   1.700 },
   { 68.960306 ,       1.28 ,     9.690 ,    8.60 ,    0.0 , -5.600 ,   1.700 },
   { 69.489021 ,       0.47 ,    10.720 ,    8.50 ,    0.0 , -5.600 ,   1.700 },
   { 70.017342 ,       0.16 ,    11.830 ,    8.40 ,    0.0 , -5.600 ,   1.700 },
  { 118.750341 ,     945.00 ,     0.000 ,   15.92 ,    0.0 , -0.440 ,   0.900 },
  { 368.498350 ,      67.90 ,     0.020 ,   19.20 ,    0.6 ,  0.000 ,   0.000 },
  { 424.763120 ,     638.00 ,     0.011 ,   19.16 ,    0.6 ,  0.000 ,   0.000 },
  { 487.249370 ,     235.00 ,     0.011 ,   19.20 ,    0.6 ,  0.000 ,   0.000 },
  { 715.393150 ,      99.60 ,     0.089 ,   18.10 ,    0.6 ,  0.000 ,   0.000 },
  { 773.838730 ,     671.00 ,     0.079 ,   18.10 ,    0.6 ,  0.000 ,   0.000 },
  { 834.145330 ,     180.00 ,     0.079 ,   18.10 ,    0.6 ,  0.000 ,   0.000 },
};

  // number of lines of Liebe O2-line catalog (0-47 lines)
  const Index i_first = 0;
  const Index i_last  = 47; // all the spec. lines up to 1THz
  // const Index i_last  = 40; // only the 60GHz complex + 118GHz line
  

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the MPM85 model (Liebe, Radio Science, 20, 1069-1089, 1985):
  const Numeric CC_MPM85 = 1.00000;
  const Numeric CL_MPM85 = 1.00000;
  const Numeric CW_MPM85 = 1.00000;
  const Numeric CO_MPM85 = 1.00000;
  int   AppCutoff = 0;
  // ---------------------------------------------------------------------------------------


  // select the parameter set (!!model dominates values!!):
  Numeric CC, CL, CW, CO;
  if ( model == "MPM85" )
    {
      CC = CC_MPM85;
      CL = CL_MPM85;
      CW = CW_MPM85;
      CO = CO_MPM85;
    }
  else if ( model == "MPM85Lines" )
    {
      CC = 0.000;
      CL = CL_MPM85;
      CW = CW_MPM85;
      CO = CO_MPM85;
    }
  else if ( model == "MPM85Continuum" )
    {
      CC = CC_MPM85;
      CL = 0.000;
      CW = 0.000;
      CO = 0.000;
    }
  else if ( model == "MPM85NoCoupling" )
    {
      CC = CC_MPM85;
      CL = CL_MPM85;
      CW = CW_MPM85;
      CO = 0.000;
    }
  else if ( model == "MPM85NoCutoff" )
    {
      CC = CC_MPM85;
      CL = CL_MPM85;
      CW = CW_MPM85;
      CO = CO_MPM85;
      AppCutoff = 1;
    }
  else if ( model == "user" )
    {
      CC = CCin;
      CL = CLin;
      CW = CWin;
      CO = COin;
    }
  else
    {
      ostringstream os;
      os << "O2-MPM85: ERROR! Wrong model values given.\n"
         << "Valid models are: 'MPM85' 'MPM85Lines' 'MPM85Continuum' 'MPM85NoCoupling' 'MPM85NoCutoff'" 
         << "and 'user'" << '\n';
      throw runtime_error(os.str());
    }
  out3  << "O2-MPM85: (model=" << model << ") parameter values in use:\n" 
        << " CC = " << CC << "\n"
        << " CL = " << CL << "\n"
        << " CW = " << CW << "\n"
        << " CO = " << CO << "\n";
  

  // O2 continuum parameters of MPM92:
  const Numeric S0 =  6.140e-4; // line strength                        [ppm]
  const Numeric G0 =  5.600e-3;  // line width                           [GHz/kPa]
  const Numeric X0 =  0.800;    // temperature dependence of line width [1]

  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // const = VMR * ISORATIO = 0.20946 * 0.99519
  // this constant is already incorporated into the line strength, so we 
  // have top devide the line strength by this value since arts multiplies xsec
  // by these variables later in absCalc.
  const Numeric VMRISO = 0.2085;

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );

  // Loop pressure/temperature (pressure in hPa therefore the factor 0.01)
  for ( Index i=0; i<n_p; ++i )
    {
      // check if O2-VMR will cause an underflow due to division by zero:
      if (vmr[i] < VMRCalcLimit)
        {
          ostringstream os;
          os << "ERROR: MPM87 O2 full absorption model has detected a O2 volume mixing ratio of " 
             << vmr[i] << " which is below the threshold of " << VMRCalcLimit << ".\n"
             << "Therefore no calculation is performed.\n";
          throw runtime_error(os.str());
          return;
        }

      // relative inverse temperature [1]
      Numeric theta     = (300.0 / t_abs[i]);
      // H2O partial pressure [kPa]
      Numeric pwv       = Pa_to_kPa * p_abs[i] * h2o_abs[i];
      // dry air partial pressure [kPa]
      Numeric pda       = (Pa_to_kPa * p_abs[i]) - pwv;
      // here the total pressure is devided by the O2 vmr for the 
      // P_dry calculation because we calculate xsec and not abs: abs = vmr * xsec
      Numeric pda_dummy = pda;
      // O2 continuum strength [ppm]
      Numeric strength_cont =  S0 * pda_dummy * pow( theta, (Numeric)2. );
      // O2 continuum pseudo line broadening [GHz]
      Numeric gam_cont      =  G0 * ( pda + 1.10*pwv ) *  pow( theta, X0 ); // GHz
      
      // Loop over input frequency
      for ( Index s=0; s<n_f; ++s )
        {
          // input frequency in [GHz]
          Numeric ff = f_mono[s] * Hz_to_GHz; 
          // O2 continuum absorption [1/m]
          // cross section: xsec = absorption / var
          // the vmr of O2 will be multiplied at the stage of absorption calculation:
          // here the rolloff parameter FAC is implemented!
          // Numeric FAC =  1.000 / ( pow( ff, 2) + pow( 60.000, 2) );
          // if we let the non-proofen rollofff away as in further version: 
          Numeric FAC =  1.000 ;
          Numeric Nppc =  CC * strength_cont * FAC * ff * gam_cont /
                          ( pow( ff, (Numeric)2.)
                            + pow( gam_cont, (Numeric)2.) );
          
          // Loop over MPM85 O2 spectral lines:
          Numeric Nppl  = 0.0;
          for ( Index l = i_first; l <= i_last; ++l )
            {
              // line strength [ppm]   S=A(1,I)*P*V**3*EXP(A(2,I)*(1.-V))*1.E-6
              Numeric strength = CL * mpm85[l][1] * 1.000e-6  * pda_dummy * 
                                      pow(theta, (Numeric)3.) * exp(mpm85[l][2]*(1.000-theta)) /
                                      mpm85[l][0];
              // line broadening parameter [GHz]
              Numeric gam      = CW * ( mpm85[l][3] * 1.000e-3 * 
                                      ( (       pda * pow(theta, ((Numeric)0.80-mpm85[l][4]))) + 
                                        (1.10 * pwv * theta) ) );
              // line mixing parameter [1]
              Numeric delta    = CO * mpm85[l][5] * 1.000e-3 * 
                                      pda * pow(theta, mpm85[l][6]);
              // absorption [dB/km] like in the original MPM92
              Nppl            += strength * MPMLineShapeO2Function(gam, mpm85[l][0], ff, delta); 
            }
          // in MPM85 there is a cutoff for O2 line absorption if abs_l < 0 
          // absorption cannot be less than 0 according to MPM87 philosophy.
          // since this cutoff is only 'detectable' in the source code and not in the
          // publications we assume this cutoff also for MPM85 since it is also 
          // implemented in MPM87. 
          if (AppCutoff == 0) 
            {
              if (Nppl < 0.000)  Nppl = 0.0000;
            }
          //
          // O2 line absorption [1/m]
          // cross section: xsec = absorption / var
          // the vmr of O2 will be multiplied at the stage of absorption calculation:
          xsec(s,i) += dB_km_to_1_m * 0.1820 * ff * (Nppl+Nppc) / VMRISO;
        }
    }
  return;
}
//
// #################################################################################
// 
void MPM87O2AbsModel( MatrixView          xsec,
                      const Numeric       CCin,       // continuum scale factor 
                      const Numeric       CLin,       // line strength scale factor
                      const Numeric       CWin,       // line broadening scale factor
                      const Numeric       COin,       // line coupling scale factor
                      const String&       model,
                      ConstVectorView     f_mono,
                      ConstVectorView     p_abs,
                      ConstVectorView     t_abs,
                      ConstVectorView     h2o_abs,
                      ConstVectorView     vmr )
{
  //
  // Coefficients are from Liebe et al., AGARD CP-May93, Paper 3/1-10
  //         0            1           2        3          4        5        6
  //         f0           a1          a2       a3         a4      a5        a6
  //        [GHz]      [kHz/hPa]     [1]    [MHz/hPa]    [1]         [1/kPa]
  const Numeric mpm87[48][7] = { 
    { 49.452379 ,       0.12 ,    11.830 ,    8.40 ,    0.0 ,  6.600 ,   1.700}, // 0
    { 49.962257 ,       0.34 ,    10.720 ,    8.50 ,    0.0 ,  6.600 ,   1.700}, // 1
    { 50.474238 ,       0.94 ,     9.690 ,    8.60 ,    0.0 ,  6.600 ,   1.700}, // 2 
    { 50.987748 ,       2.46 ,     8.690 ,    8.70 ,    0.0 ,  6.500 ,   1.700}, // 3
    { 51.503350 ,       6.08 ,     7.740 ,    8.90 ,    0.0 ,  6.627 ,   1.800}, // 4
    { 52.021409 ,      14.14 ,     6.840 ,    9.20 ,    0.0 ,  6.347 ,   1.800}, // 5
    { 52.542393 ,      31.02 ,     6.000 ,    9.40 ,    0.0 ,  6.046 ,   1.800}, // 6
    { 53.066906 ,      64.10 ,     5.220 ,    9.70 ,    0.0 ,  5.719 ,   1.900}, // 7
    { 53.595748 ,     124.70 ,     4.480 ,   10.00 ,    0.0 ,  5.400 ,   1.800}, // 8
    { 54.129999 ,     228.00 ,     3.810 ,   10.20 ,    0.0 ,  5.157 ,   2.000}, // 9
    { 54.671157 ,     391.80 ,     3.190 ,   10.50 ,    0.0 ,  4.783 ,   1.900}, // 10
    { 55.221365 ,     631.60 ,     2.620 ,   10.79 ,    0.0 ,  4.339 ,   2.100}, // 11
    { 55.783800 ,     953.50 ,     2.115 ,   11.10 ,    0.0 ,  4.011 ,   2.100}, // 12
    { 56.264777 ,     548.90 ,     0.010 ,   16.46 ,    0.0 ,  2.772 ,   0.900}, // 13
    { 56.363387 ,    1344.00 ,     1.655 ,   11.44 ,    0.0 ,  3.922 ,   2.300}, // 14
    { 56.968180 ,    1763.00 ,     1.255 ,   11.81 ,    0.0 ,  3.398 ,   2.500}, // 15
    { 57.612481 ,    2141.00 ,     0.910 ,   12.21 ,    0.0 ,  1.145 ,   3.200}, // 16
    { 58.323874 ,    2386.00 ,     0.621 ,   12.66 ,    0.0 , -0.317 ,  -2.500}, // 17
    { 58.446589 ,    1457.00 ,     0.079 ,   14.49 ,    0.0 ,  6.270 ,   0.800}, // 18
    { 59.164204 ,    2404.00 ,     0.386 ,   13.19 ,    0.0 , -4.119 ,   0.100}, // 19
    { 59.590982 ,    2112.00 ,     0.207 ,   13.60 ,    0.0 ,  6.766 ,   0.500}, // 20
    { 60.306057 ,    2124.00 ,     0.207 ,   13.82 ,    0.0 , -6.183 ,   0.700}, // 21
    { 60.434775 ,    2461.00 ,     0.386 ,   12.97 ,    0.0 ,  3.290 ,  -0.400}, // 22
    { 61.150558 ,    2504.00 ,     0.621 ,   12.48 ,    0.0 , -1.591 ,   3.500}, // 23
    { 61.800152 ,    2298.00 ,     0.910 ,   12.07 ,    0.0 , -2.068 ,   2.900}, // 24
    { 62.411212 ,    1933.00 ,     1.255 ,   11.71 ,    0.0 , -4.158 ,   2.300}, // 25
    { 62.486253 ,    1517.00 ,     0.078 ,   14.68 ,    0.0 , -4.068 ,   0.900}, // 26
    { 62.997974 ,    1503.00 ,     1.660 ,   11.39 ,    0.0 , -4.482 ,   2.200}, // 27
    { 63.568515 ,    1087.00 ,     2.110 ,   11.08 ,    0.0 , -4.442 ,   2.000}, // 28
    { 64.127764 ,     733.50 ,     2.620 ,   10.78 ,    0.0 , -4.687 ,   2.000}, // 29
    { 64.678900 ,     463.50 ,     3.190 ,   10.50 ,    0.0 , -5.074 ,   1.800}, // 30
    { 65.224067 ,     274.80 ,     3.810 ,   10.20 ,    0.0 , -5.403 ,   1.900}, // 31
    { 65.764769 ,     153.00 ,     4.480 ,   10.00 ,    0.0 , -5.610 ,   1.800}, // 32
    { 66.302088 ,      80.09 ,     5.220 ,    9.70 ,    0.0 , -5.896 ,   1.800}, // 33
    { 66.836827 ,      39.46 ,     6.000 ,    9.40 ,    0.0 , -6.194 ,   1.700}, // 34
    { 67.369595 ,      18.32 ,     6.840 ,    9.20 ,    0.0 , -6.468 ,   1.800}, // 35
    { 67.900862 ,       8.01 ,     7.740 ,    8.90 ,    0.0 , -6.718 ,   1.700}, // 36
    { 68.431001 ,       3.30 ,     8.690 ,    8.70 ,    0.0 , -6.700 ,   1.700}, // 37
    { 68.960306 ,       1.28 ,     9.690 ,    8.60 ,    0.0 , -6.600 ,   1.700}, // 38
    { 69.489021 ,       0.47 ,    10.720 ,    8.50 ,    0.0 , -6.600 ,   1.700}, // 39
    { 70.017342 ,       0.16 ,    11.830 ,    8.40 ,    0.0 , -6.600 ,   1.700}, // 40
   { 118.750341 ,     945.00 ,     0.000 ,   16.30 ,    0.0 , -0.134 ,   0.800}, // 41
  {  368.498350 ,      67.90 ,     0.020 ,   19.20 ,    0.6 ,  0.000 ,   0.000}, // 42
  {  424.763120 ,     638.00 ,     0.011 ,   19.16 ,    0.6 ,  0.000 ,   0.000}, // 43
  {  487.249370 ,     235.00 ,     0.011 ,   19.20 ,    0.6 ,  0.000 ,   0.000}, // 44
  {  715.393150 ,      99.60 ,     0.089 ,   18.10 ,    0.6 ,  0.000 ,   0.000}, // 45
  {  773.838730 ,     671.00 ,     0.079 ,   18.10 ,    0.6 ,  0.000 ,   0.000}, // 46
  {  834.145330 ,     180.00 ,     0.079 ,   18.10 ,    0.6 ,  0.000 ,   0.000}  // 47
  };

  // number of lines of Liebe O2-line catalog (0-47 lines)
  const Index i_first = 0;
  const Index i_last  = 47; // all the spec. lines up to 1THz
  // const Index i_last  = 40; // only the 60GHz complex + 118GHz line
  

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the MPM87 model (NITA Report 87-224):
  const Numeric CC_MPM87 = 1.00000;
  const Numeric CL_MPM87 = 1.00000;
  const Numeric CW_MPM87 = 1.00000;
  const Numeric CO_MPM87 = 1.00000;
  int   AppCutoff = 0;
  // ---------------------------------------------------------------------------------------


  // select the parameter set (!!model dominates values!!):
  Numeric CC, CL, CW, CO;
  if ( model == "MPM87" )
    {
      CC = CC_MPM87;
      CL = CL_MPM87;
      CW = CW_MPM87;
      CO = CO_MPM87;
    }
  else if ( model == "MPM87Lines" )
    {
      CC = 0.000;
      CL = CL_MPM87;
      CW = CW_MPM87;
      CO = CO_MPM87;
    }
  else if ( model == "MPM87Continuum" )
    {
      CC = CC_MPM87;
      CL = 0.000;
      CW = 0.000;
      CO = 0.000;
    }
  else if ( model == "MPM87NoCoupling" )
    {
      CC = CC_MPM87;
      CL = CL_MPM87;
      CW = CW_MPM87;
      CO = 0.000;
    }
  else if ( model == "MPM87NoCutoff" )
    {
      // !!ATTENTION!!
      // In the window regions the total absorption can get negative values.
      // So be carefull with this selection!
      CC = CC_MPM87;
      CL = CL_MPM87;
      CW = CW_MPM87;
      CO = CO_MPM87;
      AppCutoff = 1;
    }
  else if ( model == "user" )
    {
      CC = CCin;
      CL = CLin;
      CW = CWin;
      CO = COin;
    }
  else
    {
      ostringstream os;
      os << "O2-MPM87: ERROR! Wrong model values given.\n"
         << "Valid models are: 'MPM87' 'MPM87Lines' 'MPM87Continuum' 'MPM87NoCoupling' 'MPM87NoCutoff'" 
         << "and 'user'" << '\n';
      throw runtime_error(os.str());
    }
  out3  << "O2-MPM87: (model=" << model << ") parameter values in use:\n" 
        << " CC = " << CC << "\n"
        << " CL = " << CL << "\n"
        << " CW = " << CW << "\n"
        << " CO = " << CO << "\n";
  

  // O2 continuum parameters of MPM92:
  const Numeric S0 =  6.140e-4; // line strength                        [ppm]
  const Numeric G0 =  4.800e-3;  // line width [GHz/kPa] !! 14% lower than in all the other versions !!
  const Numeric X0 =  0.800;    // temperature dependence of line width [1]

  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // const = VMR * ISORATIO = 0.20946 * 0.99519
  // this constant is already incorporated into the line strength, so we 
  // have top devide the line strength by this value since arts multiplies xsec
  // by these variables later in absCalc.
  const Numeric VMRISO = 0.2085;

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );

  // Loop pressure/temperature (pressure in hPa therefore the factor 0.01)
  for ( Index i=0; i<n_p; ++i )
    {
      // check if O2-VMR will cause an underflow due to division by zero:
      if (vmr[i] < VMRCalcLimit)
        {
          ostringstream os;
          os << "ERROR: MPM87 O2 full absorption model has detected a O2 volume mixing ratio of " 
             << vmr[i] << " which is below the threshold of " << VMRCalcLimit << ".\n"
             << "Therefore no calculation is performed.\n";
          throw runtime_error(os.str());
          return;
        }

      // relative inverse temperature [1]
      Numeric theta     = (300.0 / t_abs[i]);
      // H2O partial pressure [kPa]
      Numeric pwv       = Pa_to_kPa * p_abs[i] * h2o_abs[i];
      // dry air partial pressure [kPa]
      Numeric pda       = (Pa_to_kPa * p_abs[i]) - pwv;
      // here the total pressure is devided by the O2 vmr for the 
      // P_dry calculation because we calculate xsec and not abs: abs = vmr * xsec
      Numeric pda_dummy = pda;
      // O2 continuum strength [ppm]
      Numeric strength_cont =  S0 * pda_dummy * pow( theta, (Numeric)2. );
      // O2 continuum pseudo line broadening [GHz]
      Numeric gam_cont      =  G0 * ( pda + 1.10*pwv ) *  pow( theta, X0 ); // GHz
      
      // Loop over input frequency
      for ( Index s=0; s<n_f; ++s )
        {
          // input frequency in [GHz]
          Numeric ff = f_mono[s] * Hz_to_GHz; 
          // O2 continuum absorption [1/m]
          // cross section: xsec = absorption / var
          // the vmr of O2 will be multiplied at the stage of absorption calculation:
          Numeric Nppc =  CC * strength_cont * ff * gam_cont /
                          ( pow( ff, (Numeric)2.) + pow( gam_cont, (Numeric)2.) );
          
          // Loop over MPM87 O2 spectral lines:
          Numeric Nppl  = 0.0;
          for ( Index l = i_first; l <= i_last; ++l )
            {
              // line strength [ppm]   S=A(1,I)*P*V**3*EXP(A(2,I)*(1.-V))*1.E-6
              Numeric strength = CL * mpm87[l][1] * 1.000e-6  * pda_dummy * 
                                      pow(theta, (Numeric)3.) * exp(mpm87[l][2]*(1.000-theta)) /
                                      mpm87[l][0];
              // line broadening parameter [GHz]
              Numeric gam      = CW * ( mpm87[l][3] * 1.000e-3 * 
                                      ( (       pda * pow(theta, ((Numeric)0.80-mpm87[l][4]))) + 
                                        (1.10 * pwv * theta) ) );
              // line mixing parameter [1]
              Numeric delta    = CO * mpm87[l][5] * 1.000e-3 * 
                                      pda * pow(theta, mpm87[l][6]);
              // absorption [dB/km] like in the original MPM92
              Nppl            += strength * MPMLineShapeO2Function(gam, mpm87[l][0], ff, delta); 
            }
          // in MPM87 there is a cutoff for O2 line absorption if abs_l < 0 
          // absorption cannot be less than 0 according to MPM87 source code.
          if (AppCutoff == 0) 
            {
              if (Nppl < 0.000)  Nppl = 0.0000;
            }
          //
          // O2 line absorption [1/m]
          // cross section: xsec = absorption / var
          // the vmr of O2 will be multiplied at the stage of absorption calculation:
          xsec(s,i) += dB_km_to_1_m * 0.1820 * ff * (Nppl+Nppc) / VMRISO;
        }
    }
  return;
}
//
// #################################################################################
// 
void MPM89O2AbsModel( MatrixView          xsec,
                      const Numeric       CCin,       // continuum scale factor 
                      const Numeric       CLin,       // line strength scale factor
                      const Numeric       CWin,       // line broadening scale factor
                      const Numeric       COin,       // line coupling scale factor
                      const String&       model,
                      ConstVectorView     f_mono,
                      ConstVectorView     p_abs,
                      ConstVectorView     t_abs,
                      ConstVectorView     h2o_abs,
                      ConstVectorView     vmr )
{
  //
  // Coefficients are from Liebe et al., AGARD CP-May93, Paper 3/1-10
  //         0            1           2        3          4        5        6
  //         f0           a1          a2       a3         a4      a5        a6
  //        [GHz]      [kHz/hPa]     [1]    [MHz/hPa]    [1]         [1/kPa]
  const Numeric mpm89[44][7] = { 
    {   50.474238,        0.94 ,    9.694 ,    8.60 ,    0.0 ,  1.600 ,   5.520 }, // 0
    {   50.987749,        2.46 ,    8.694 ,    8.70 ,    0.0 ,  1.400 ,   5.520 }, // 1
    {   51.503350,        6.08 ,    7.744 ,    8.90 ,    0.0 ,  1.165 ,   5.520 }, // 2
    {   52.021410,       14.14 ,    6.844 ,    9.20 ,    0.0 ,  0.883 ,   5.520 }, // 3
    {   52.542394,       31.02 ,    6.004 ,    9.40 ,    0.0 ,  0.579 ,   5.520 }, // 4
    {   53.066907,       64.10 ,    5.224 ,    9.70 ,    0.0 ,  0.252 ,   5.520 }, // 5
    {   53.595749,      124.70 ,    4.484 ,   10.00 ,    0.0 , -0.066 ,   5.520 }, // 6
    {   54.130000,      228.00 ,    3.814 ,   10.20 ,    0.0 , -0.314 ,   5.520 }, // 7
    {   54.671159,      391.80 ,    3.194 ,   10.50 ,    0.0 , -0.706 ,   5.520 }, // 8
    {   55.221367,      631.60 ,    2.624 ,   10.79 ,    0.0 , -1.151 ,   5.514 }, // 9
    {   55.783802,      953.50 ,    2.119 ,   11.10 ,    0.0 , -0.920 ,   5.025 }, // 10
    {   56.264775,      548.90 ,    0.015 ,   16.46 ,    0.0 ,  2.881 ,  -0.069 }, // 11
    {   56.363389,     1344.00 ,    1.660 ,   11.44 ,    0.0 , -0.596 ,   4.750 }, // 12
    {   56.968206,     1763.00 ,    1.260 ,   11.81 ,    0.0 , -0.556 ,   4.104 }, // 13
    {   57.612484,     2141.00 ,    0.915 ,   12.21 ,    0.0 , -2.414 ,   3.536 }, // 14
    {   58.323877,     2386.00 ,    0.626 ,   12.66 ,    0.0 , -2.635 ,   2.686 }, // 15
    {   58.446590,     1457.00 ,    0.084 ,   14.49 ,    0.0 ,  6.848 ,  -0.647 }, // 16
    {   59.164207,     2404.00 ,    0.391 ,   13.19 ,    0.0 , -6.032 ,   1.858 }, // 17
    {   59.590983,     2112.00 ,    0.212 ,   13.60 ,    0.0 ,  8.266 ,  -1.413 }, // 18
    {   60.306061,     2124.00 ,    0.212 ,   13.82 ,    0.0 , -7.170 ,   0.916 }, // 19
    {   60.434776,     2461.00 ,    0.391 ,   12.97 ,    0.0 ,  5.664 ,  -2.323 }, // 20
    {   61.150560,     2504.00 ,    0.626 ,   12.48 ,    0.0 ,  1.731 ,  -3.039 }, // 21
    {   61.800154,     2298.00 ,    0.915 ,   12.07 ,    0.0 ,  1.738 ,  -3.797 }, // 22
    {   62.411215,     1933.00 ,    1.260 ,   11.71 ,    0.0 , -0.048 ,  -4.277 }, // 23
    {   62.486260,     1517.00 ,    0.083 ,   14.68 ,    0.0 , -4.290 ,   0.238 }, // 24
    {   62.997977,     1503.00 ,    1.665 ,   11.39 ,    0.0 ,  0.134 ,  -4.860 }, // 25
    {   63.568518,     1087.00 ,    2.115 ,   11.08 ,    0.0 ,  0.541 ,  -5.079 }, // 26
    {   64.127767,      733.50 ,    2.620 ,   10.78 ,    0.0 ,  0.814 ,  -5.525 }, // 27
    {   64.678903,      463.50 ,    3.195 ,   10.50 ,    0.0 ,  0.415 ,  -5.520 }, // 28
    {   65.224071,      274.80 ,    3.815 ,   10.20 ,    0.0 ,  0.069 ,  -5.520 }, // 29
    {   65.764772,      153.00 ,    4.485 ,   10.00 ,    0.0 , -0.143 ,  -5.520 }, // 30
    {   66.302091,       80.09 ,    5.225 ,    9.70 ,    0.0 , -0.428 ,  -5.520 }, // 31
    {   66.836830,       39.46 ,    6.005 ,    9.40 ,    0.0 , -0.726 ,  -5.520 }, // 32
    {   67.369598,       18.32 ,    6.845 ,    9.20 ,    0.0 , -1.002 ,  -5.520 }, // 33
    {   67.900867,        8.01 ,    7.745 ,    8.90 ,    0.0 , -1.255 ,  -5.520 }, // 34
    {   68.431005,        3.30 ,    8.695 ,    8.70 ,    0.0 , -1.500 ,  -5.520 }, // 35
    {   68.960311,        1.28 ,    9.695 ,    8.60 ,    0.0 , -1.700 ,  -5.520 }, // 36
    {  118.750343,      945.00 ,    0.009 ,   16.30 ,    0.0 , -0.247 ,   0.003 }, // 37
    {  368.498350,       67.90 ,    0.049 ,   19.20 ,    0.6 ,  0.000 ,   0.000 }, // 38
    {  424.763124,      638.00 ,    0.044 ,   19.16 ,    0.6 ,  0.000 ,   0.000 }, // 39
    {  487.249370,      235.00 ,    0.049 ,   19.20 ,    0.6 ,  0.000 ,   0.000 }, // 40
    {  715.393150,       99.60 ,    0.145 ,   18.10 ,    0.6 ,  0.000 ,   0.000 }, // 41
    {  773.839675,      671.00 ,    0.130 ,   18.10 ,    0.6 ,  0.000 ,   0.000 }, // 42
    {  834.145330,      180.00 ,    0.147 ,   18.10 ,    0.6 ,  0.000 ,   0.000 }  // 43
  };

  // number of lines of Liebe O2-line catalog (0-43 lines)
  const Index i_first = 0;
  const Index i_last  = 43; // all the spec. lines up to 1THz
  // const Index i_last  = 37; // only the 60GHz complex + 118GHz line
  

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the MPM89 model (IJIMW, Vol 10, pp. 631-650, 1989):
  const Numeric CC_MPM89 = 1.00000;
  const Numeric CL_MPM89 = 1.00000;
  const Numeric CW_MPM89 = 1.00000;
  const Numeric CO_MPM89 = 1.00000;
  int   AppCutoff = 0; 
  // ---------------------------------------------------------------------------------------


  // select the parameter set (!!model dominates values!!):
  Numeric CC, CL, CW, CO;
  if ( model == "MPM89" )
    {
      CC = CC_MPM89;
      CL = CL_MPM89;
      CW = CW_MPM89;
      CO = CO_MPM89;
    }
  else if ( model == "MPM89Lines" )
    {
      CC = 0.000;
      CL = CL_MPM89;
      CW = CW_MPM89;
      CO = CO_MPM89;
    }
  else if ( model == "MPM89Continuum" )
    {
      CC = CC_MPM89;
      CL = 0.000;
      CW = 0.000;
      CO = 0.000;
    }
  else if ( model == "MPM89NoCoupling" )
    {
      CC = CC_MPM89;
      CL = CL_MPM89;
      CW = CW_MPM89;
      CO = 0.000;
    }
  else if ( model == "MPM89NoCutoff" )
    {
      CC = CC_MPM89;
      CL = CL_MPM89;
      CW = CW_MPM89;
      CO = CO_MPM89;
      AppCutoff = 1; 
    }
  else if ( model == "user" )
    {
      CC = CCin;
      CL = CLin;
      CW = CWin;
      CO = COin;
    }
  else
    {
      ostringstream os;
      os << "O2-MPM89: ERROR! Wrong model values given.\n"
         << "Valid models are: 'MPM89' 'MPM89Lines' 'MPM89Continuum' 'MPM89NoCoupling' 'MPM89NoCutoff'" 
         << "and 'user'" << '\n';
      throw runtime_error(os.str());
    }
  out3  << "O2-MPM89: (model=" << model << ") parameter values in use:\n" 
        << " CC = " << CC << "\n"
        << " CL = " << CL << "\n"
        << " CW = " << CW << "\n"
        << " CO = " << CO << "\n";
  

  // O2 continuum parameters of MPM92:
  const Numeric S0 =  6.140e-4; // line strength                        [ppm]
  const Numeric G0 =  5.60e-3;  // line width                           [GHz/kPa]
  const Numeric X0 =  0.800;    // temperature dependence of line width [1]

  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // const = VMR * ISORATIO = 0.20946 * 0.99519
  // this constant is already incorporated into the line strength, so we 
  // have top devide the line strength by this value since arts multiplies xsec
  // by these variables later in absCalc.
  const Numeric VMRISO = 0.2085;

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );

  // Loop pressure/temperature (pressure in hPa therefore the factor 0.01)
  for ( Index i=0; i<n_p; ++i )
    {
      // check if O2-VMR will cause an underflow due to division by zero:
      if (vmr[i] < VMRCalcLimit)
        {
          ostringstream os;
          os << "ERROR: MPM89 O2 full absorption model has detected a O2 volume mixing ratio of " 
             << vmr[i] << " which is below the threshold of " << VMRCalcLimit << ".\n"
             << "Therefore no calculation is performed.\n";
          throw runtime_error(os.str());
          return;
        }

      // relative inverse temperature [1]
      Numeric theta     = (300.0 / t_abs[i]);
      // H2O partial pressure [kPa]
      Numeric pwv       = Pa_to_kPa * p_abs[i] * h2o_abs[i];
      // dry air partial pressure [kPa]
      Numeric pda       = (Pa_to_kPa * p_abs[i]) - pwv;
      // here the total pressure is devided by the O2 vmr for the 
      // P_dry calculation because we calculate xsec and not abs: abs = vmr * xsec
      Numeric pda_dummy = pda;
      // O2 continuum strength [ppm]
      Numeric strength_cont =  S0 * pda_dummy * pow( theta, (Numeric)2. );
      // O2 continuum pseudo line broadening [GHz]
      Numeric gam_cont      =  G0 * (pwv+pda) *  pow( theta, X0 ); // GHz
      
      // Loop over input frequency
      for ( Index s=0; s<n_f; ++s )
        {
          // input frequency in [GHz]
          Numeric ff = f_mono[s] * Hz_to_GHz; 
          // O2 continuum absorption [1/m]
          // cross section: xsec = absorption / var
          // the vmr of O2 will be multiplied at the stage of absorption calculation:
          Numeric Nppc =  CC * strength_cont * ff * gam_cont /
                          ( pow( ff, (Numeric)2.) + pow( gam_cont, (Numeric)2.) );
          
          // Loop over MPM89 O2 spectral lines:
          Numeric Nppl  = 0.0;
          for ( Index l = i_first; l <= i_last; ++l )
            {
              // line strength [ppm]   S=A(1,I)*P*V**3*EXP(A(2,I)*(1.-V))*1.E-6
              Numeric strength = CL * mpm89[l][1] * 1.000e-6  * pda_dummy * 
                                      pow(theta, (Numeric)3.) * exp(mpm89[l][2]*(1.000-theta)) /
                                      mpm89[l][0];
              // line broadening parameter [GHz]
              Numeric gam      = CW * ( mpm89[l][3] * 1.000e-3 * 
                                      ( (       pda * pow(theta, ((Numeric)0.80-mpm89[l][4]))) + 
                                        (1.10 * pwv * theta) ) );
              // line mixing parameter [1]
              Numeric delta    = CO * ( (mpm89[l][5] + mpm89[l][6] * theta) * 1.000e-3 * 
                                        pda * pow(theta, (Numeric)0.8) );
              // absorption [dB/km] like in the original MPM92
              Nppl            += strength * MPMLineShapeO2Function(gam, mpm89[l][0], ff, delta); 
            }
          // in MPM89 we adopt the cutoff for O2 line absorption if abs_l < 0 
          // absorption cannot be less than 0 according to MPM87 source code.
          if (AppCutoff == 0) 
            {
              if (Nppl < 0.000)  Nppl = 0.0000;
            }
          //
          // O2 line absorption [1/m]
          // cross section: xsec = absorption / var
          // the vmr of O2 will be multiplied at the stage of absorption calculation:
          xsec(s,i) += dB_km_to_1_m * 0.1820 * ff * (Nppl+Nppc) / VMRISO;
        }
    }
  return;
}
//
// #################################################################################
// 
//
void MPM92O2AbsModel( MatrixView          xsec,
                      const Numeric       CCin,       // continuum scale factor 
                      const Numeric       CLin,       // line strength scale factor
                      const Numeric       CWin,       // line broadening scale factor
                      const Numeric       COin,       // line coupling scale factor
                      const String&       model,
                      ConstVectorView     f_mono,
                      ConstVectorView     p_abs,
                      ConstVectorView     t_abs,
                      ConstVectorView     h2o_abs,
                      ConstVectorView     vmr )
{
  //
  // Coefficients are from Liebe et al., AGARD CP-May93, Paper 3/1-10
  //         0           1            2       3        4      5      6
  //         f0          a1           a2      a3       a4     a5     a6
  //        [GHz]     [kHz/hPa]      [1]   [MHz/hPa]  [1]    [10³/hPa]
  const Numeric mpm92[44][7] = { 
    {   50.474238,       0.094,      9.694,    0.850,     0.0,   0.210,    0.685}, // 0
    {   50.987749,       0.246,      8.694,    0.870,     0.0,   0.190,    0.680}, // 1
    {   51.503350,       0.608,      7.744,    0.890,     0.0,   0.171,    0.673}, // 2 
    {   52.021410,       1.414,      6.844,    0.920,     0.0,   0.144,    0.664}, // 3
    {   52.542394,       3.102,      6.004,    0.940,     0.0,   0.118,    0.653}, // 4
    {   53.066907,       6.410,      5.224,    0.970,     0.0,   0.114,    0.621}, // 5
    {   53.595749,      12.470,      4.484,    1.000,     0.0,   0.200,    0.508}, // 6
    {   54.130000,      22.800,      3.814,    1.020,     0.0,   0.291,    0.375}, // 7
    {   54.671159,      39.180,      3.194,    1.050,     0.0,   0.325,    0.265}, // 8
    {   55.221367,      63.160,      2.624,    1.080,     0.0,   0.224,    0.295}, // 9
    {   55.783802,      95.350,      2.119,    1.110,     0.0,  -0.144,    0.613}, // 0
    {   56.264775,      54.890,      0.015,    1.646,     0.0,   0.339,   -0.098}, // 11
    {   56.363389,     134.400,      1.660,    1.144,     0.0,  -0.258,    0.655}, // 12
    {   56.968206,     176.300,      1.260,    1.181,     0.0,  -0.362,    0.645}, // 13
    {   57.612484,     214.100,      0.915,    1.221,     0.0,  -0.533,    0.606}, // 14
    {   58.323877,     238.600,      0.626,    1.266,     0.0,  -0.178,    0.044}, // 15
    {   58.446590,     145.700,      0.084,    1.449,     0.0,   0.650,   -0.127}, // 16
    {   59.164207,     240.400,      0.391,    1.319,     0.0,  -0.628,    0.231}, // 17
    {   59.590983,     211.200,      0.212,    1.360,     0.0,   0.665,   -0.078}, // 18
    {   60.306061,     212.400,      0.212,    1.382,     0.0,  -0.613,    0.070}, // 19
    {   60.434776,     246.100,      0.391,    1.297,     0.0,   0.606,   -0.282}, // 20
    {   61.150560,     250.400,      0.626,    1.248,     0.0,   0.090,   -0.058}, // 21
    {   61.800154,     229.800,      0.915,    1.207,     0.0,   0.496,   -0.662}, // 22
    {   62.411215,     193.300,      1.260,    1.171,     0.0,   0.313,   -0.676}, // 23
    {   62.486260,     151.700,      0.083,    1.468,     0.0,  -0.433,    0.084}, // 24
    {   62.997977,     150.300,      1.665,    1.139,     0.0,   0.208,   -0.668}, // 25
    {   63.568518,     108.700,      2.115,    1.110,     0.0,   0.094,   -0.614}, // 26
    {   64.127767,      73.350,      2.620,    1.080,     0.0,  -0.270,   -0.289}, // 27
    {   64.678903,      46.350,      3.195,    1.050,     0.0,  -0.366,   -0.259}, // 28
    {   65.224071,      27.480,      3.815,    1.020,     0.0,  -0.326,   -0.368}, // 29
    {   65.764772,      15.300,      4.485,    1.000,     0.0,  -0.232,   -0.500}, // 30
    {   66.302091,       8.009,      5.225,    0.970,     0.0,  -0.146,   -0.609}, // 31
    {   66.836830,       3.946,      6.005,    0.940,     0.0,  -0.147,   -0.639}, // 32
    {   67.369598,       1.832,      6.845,    0.920,     0.0,  -0.174,   -0.647}, // 33
    {   67.900867,       0.801,      7.745,    0.890,     0.0,  -0.198,   -0.655}, // 34
    {   68.431005,       0.330,      8.695,    0.870,     0.0,  -0.210,   -0.660}, // 35
    {   68.960311,       0.128,      9.695,    0.850,     0.0,  -0.220,   -0.665}, // 36
    {  118.750343,      94.500,      0.009,    1.630,     0.0,  -0.031,    0.008}, // 37
    {  368.498350,       6.790,      0.049,    1.920,     0.6,   0.000,    0.000}, // 38
    {  424.763124,      63.800,      0.044,    1.926,     0.6,   0.000,    0.000}, // 39
    {  487.249370,      23.500,      0.049,    1.920,     0.6,   0.000,    0.000}, // 40
    {  715.393150,       9.960,      0.145,    1.810,     0.6,   0.000,    0.000}, // 41
    {  773.839675,      67.100,      0.130,    1.810,     0.6,   0.000,    0.000}, // 42
    {  834.145330,      18.000,      0.147,    1.810,     0.6,   0.000,    0.000}}; // 43

  // number of lines of Liebe O2-line catalog (0-43 lines)
  const Index i_first = 0;
  const Index i_last  = 43; // all the spec. lines up to 1THz
  // const Index i_last  = 37; // only the 60GHz complex + 118GHz line
  

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the MPM92 model (JQSRT, Vol 48, pp. 629-643, 1992):
  const Numeric CC_MPM92 = 1.00000;
  const Numeric CL_MPM92 = 1.00000;
  const Numeric CW_MPM92 = 1.00000;
  const Numeric CO_MPM92 = 1.00000;
  int AppCutoff = 0;
  // ---------------------------------------------------------------------------------------


  // select the parameter set (!!model dominates values!!):
  Numeric CC, CL, CW, CO;
  if ( model == "MPM92" )
    {
      CC = CC_MPM92;
      CL = CL_MPM92;
      CW = CW_MPM92;
      CO = CO_MPM92;
    }
  else if ( model == "MPM92Lines" )
    {
      CC = 0.000;
      CL = CL_MPM92;
      CW = CW_MPM92;
      CO = CO_MPM92;
    }
  else if ( model == "MPM92Continuum" )
    {
      CC = CC_MPM92;
      CL = 0.000;
      CW = 0.000;
      CO = 0.000;
    }
  else if ( model == "MPM92NoCoupling" )
    {
      CC = CC_MPM92;
      CL = CL_MPM92;
      CW = CW_MPM92;
      CO = 0.000;
    }
  else if ( model == "MPM92NoCutoff" )
    {
      CC = CC_MPM92;
      CL = CL_MPM92;
      CW = CW_MPM92;
      CO = CO_MPM92;
      AppCutoff = 1;
    }
  else if ( model == "user" )
    {
      CC = CCin;
      CL = CLin;
      CW = CWin;
      CO = COin;
    }
  else
    {
      ostringstream os;
      os << "O2-MPM92: ERROR! Wrong model values given.\n"
         << "Valid models are: 'MPM92' 'MPM92Lines' 'MPM92Continuum' 'MPM92NoCoupling' 'MPM92NoCutoff'" 
         << "and 'user'" << '\n';
      throw runtime_error(os.str());
    }
  out3  << "O2-MPM92: (model=" << model << ") parameter values in use:\n" 
        << " CC = " << CC << "\n"
        << " CL = " << CL << "\n"
        << " CW = " << CW << "\n"
        << " CO = " << CO << "\n";
  

  // const = VMR * ISORATIO = 0.20946 * 0.99519
  // this constant is already incorporated into the line strength, so we 
  // have top devide the line strength by this value since arts multiplies xsec
  // by these variables later in absCalc.
  const Numeric VMRISO = 0.2085;

  // O2 continuum parameters of MPM92:
  const Numeric S0 =  6.140e-5; // line strength                        [ppm]
  const Numeric G0 =  0.560e-3; // line width                           [GHz/hPa]
  const Numeric X0 =  0.800;    // temperature dependence of line width [1]

  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );

  // Loop pressure/temperature (pressure in hPa therefore the factor 0.01)
  for ( Index i=0; i<n_p; ++i )
    {
      // check if O2-VMR will cause an underflow due to division by zero:
      if (vmr[i] < VMRCalcLimit)
        {
          ostringstream os;
          os << "ERROR: MPM92 O2 full absorption model has detected a O2 volume mixing ratio of " 
             << vmr[i] << " which is below the threshold of " << VMRCalcLimit << ".\n"
             << "Therefore no calculation is performed.\n";
          throw runtime_error(os.str());
          return;
        }

      // relative inverse temperature [1]
      Numeric theta     = (300.0 / t_abs[i]);
      // H2O partial pressure [hPa]
      Numeric pwv       = Pa_to_hPa * p_abs[i] * h2o_abs[i];
      // dry air partial pressure [hPa]
      Numeric pda       = (Pa_to_hPa * p_abs[i]) - pwv;
      // here the total pressure is devided by the O2 vmr for the 
      // P_dry calculation because we calculate xsec and not abs: abs = vmr * xsec
      Numeric pda_dummy = pda;
      // O2 continuum strength [ppm]
      Numeric strength_cont =  S0 * pda_dummy * pow( theta, (Numeric)2. );
      // O2 continuum pseudo line broadening [GHz]
      Numeric gam_cont      =  G0 * (pwv+pda) *  pow( theta, X0 ); // GHz
      
      // Loop over input frequency
      for ( Index s=0; s<n_f; ++s )
        {
          // input frequency in [GHz]
          Numeric ff = f_mono[s] * Hz_to_GHz; 
          // O2 continuum absorption [1/m]
          // cross section: xsec = absorption / var
          // the vmr of O2 will be multiplied at the stage of absorption calculation:
          Numeric Nppc =  CC * strength_cont * ff * gam_cont /
                          ( pow( ff, (Numeric)2.) + pow( gam_cont, (Numeric)2.) );
          
          // Loop over MPM92 O2 spectral lines:
          Numeric Nppl  = 0.0;
          for ( Index l = i_first; l <= i_last; ++l )
            {
              // line strength [ppm]   S=A(1,I)*P*V**3*EXP(A(2,I)*(1.-V))*1.E-6
              Numeric strength = CL * 1.000e-6  * pda_dummy * mpm92[l][1] / mpm92[l][0] * 
                                      pow(theta, (Numeric)3.) * exp(mpm92[l][2]*(1.0-theta));
              // line broadening parameter [GHz]
              Numeric gam      = CW * ( mpm92[l][3] * 0.001 * 
                                      ( (       pda * pow(theta, ((Numeric)0.8-mpm92[l][4]))) + 
                                        (1.10 * pwv * theta) ) );
              // line mixing parameter [1]
              //                  if (l < 11) CD = 1.1000;
              Numeric delta    = CO * ( (mpm92[l][5] + mpm92[l][6] * theta) * 
                                      (pda+pwv) * 0.001 * pow(theta, (Numeric)0.8) );
              // absorption [dB/km] like in the original MPM92
              Nppl            += strength * MPMLineShapeO2Function(gam, mpm92[l][0], ff, delta); 
            }
          // in MPM92 we adopt the cutoff for O2 line absorption if abs_l < 0 
          // absorption cannot be less than 0 according to MPM87 and MPM93 source code.
          if (AppCutoff == 0) 
            {
              if (Nppl < 0.000)  Nppl = 0.0000;
            }
          //
          // O2 line absorption [1/m]
          // cross section: xsec = absorption / var
          // the vmr of O2 will be multiplied at the stage of absorption calculation:
          xsec(s,i) += dB_km_to_1_m * 0.1820 * ff * (Nppl+Nppc) / VMRISO;
        }
    }
  return;
}
//
// #################################################################################
// 
void MPM93O2AbsModel( MatrixView          xsec,
                      const Numeric       CCin,       // continuum scale factor 
                      const Numeric       CLin,       // line strength scale factor
                      const Numeric       CWin,       // line broadening scale factor
                      const Numeric       COin,       // line coupling scale factor
                      const String&       model,
                      ConstVectorView     f_mono,
                      ConstVectorView     p_abs,
                      ConstVectorView     t_abs,
                      ConstVectorView     h2o_abs,    // VMR 0f H2O
                      ConstVectorView     vmr )       // VMR of O2
{
  //
  // Coefficients are from Liebe et al., AGARD CP-May93, Paper 3/1-10
  //         0             1           2         3         4      5        6
  //         f0           a1           a2       a3        a4      a5       a6
  //        [GHz]      [kHz/hPa]      [1]    [MHz/hPa]    [1]       [10³/hPa]
  const Numeric mpm93[44][7] = { 
    {   50.474238,       0.094,      9.694,    0.890,     0.0,   0.240,    0.790}, // 0
    {   50.987749,       0.246,      8.694,    0.910,     0.0,   0.220,    0.780}, // 1
    {   51.503350,       0.608,      7.744,    0.940,     0.0,   0.197,    0.774}, // 2 
    {   52.021410,       1.414,      6.844,    0.970,     0.0,   0.166,    0.764}, // 3
    {   52.542394,       3.102,      6.004,    0.990,     0.0,   0.136,    0.751}, // 4
    {   53.066907,       6.410,      5.224,    1.020,     0.0,   0.131,    0.714}, // 5
    {   53.595749,      12.470,      4.484,    1.050,     0.0,   0.230,    0.584}, // 6
    {   54.130000,      22.800,      3.814,    1.070,     0.0,   0.335,    0.431}, // 7
    {   54.671159,      39.180,      3.194,    1.100,     0.0,   0.374,    0.305}, // 8
    {   55.221367,      63.160,      2.624,    1.130,     0.0,   0.258,    0.339}, // 9
    {   55.783802,      95.350,      2.119,    1.170,     0.0,  -0.166,    0.705}, // 10
    {   56.264775,      54.890,      0.015,    1.730,     0.0,   0.390,   -0.113}, // 11
    {   56.363389,     134.400,      1.660,    1.200,     0.0,  -0.297,    0.753}, // 12
    {   56.968206,     176.300,      1.260,    1.240,     0.0,  -0.416,    0.742}, // 13
    {   57.612484,     214.100,      0.915,    1.280,     0.0,  -0.613,    0.697}, // 14
    {   58.323877,     238.600,      0.626,    1.330,     0.0,  -0.205,    0.051}, // 15
    {   58.446590,     145.700,      0.084,    1.520,     0.0,   0.748,   -0.146}, // 16
    {   59.164207,     240.400,      0.391,    1.390,     0.0,  -0.722,    0.266}, // 17
    {   59.590983,     211.200,      0.212,    1.430,     0.0,   0.765,   -0.090}, // 18
    {   60.306061,     212.400,      0.212,    1.450,     0.0,  -0.705,    0.081}, // 19
    {   60.434776,     246.100,      0.391,    1.360,     0.0,   0.697,   -0.324}, // 20
    {   61.150560,     250.400,      0.626,    1.310,     0.0,   0.104,   -0.067}, // 21
    {   61.800154,     229.800,      0.915,    1.270,     0.0,   0.570,   -0.761}, // 22
    {   62.411215,     193.300,      1.260,    1.230,     0.0,   0.360,   -0.777}, // 23
    {   62.486260,     151.700,      0.083,    1.540,     0.0,  -0.498,    0.097}, // 24
    {   62.997977,     150.300,      1.665,    1.200,     0.0,   0.239,   -0.768}, // 25
    {   63.568518,     108.700,      2.115,    1.170,     0.0,   0.108,   -0.706}, // 26
    {   64.127767,      73.350,      2.620,    1.130,     0.0,  -0.311,   -0.332}, // 27
    {   64.678903,      46.350,      3.195,    1.100,     0.0,  -0.421,   -0.298}, // 28
    {   65.224071,      27.480,      3.815,    1.070,     0.0,  -0.375,   -0.423}, // 29
    {   65.764772,      15.300,      4.485,    1.050,     0.0,  -0.267,   -0.575}, // 30
    {   66.302091,       8.009,      5.225,    1.020,     0.0,  -0.168,   -0.700}, // 31
    {   66.836830,       3.946,      6.005,    0.990,     0.0,  -0.169,   -0.735}, // 32
    {   67.369598,       1.832,      6.845,    0.970,     0.0,  -0.200,   -0.744}, // 33
    {   67.900867,       0.801,      7.745,    0.940,     0.0,  -0.228,   -0.753}, // 34
    {   68.431005,       0.330,      8.695,    0.920,     0.0,  -0.240,   -0.760}, // 35
    {   68.960311,       0.128,      9.695,    0.900,     0.0,  -0.250,   -0.765}, // 36
    {  118.750343,      94.500,      0.009,    1.630,     0.0,  -0.036,    0.009}, // 37
    {  368.498350,       6.790,      0.049,    1.920,     0.6,   0.000,    0.000}, // 38
    {  424.763124,      63.800,      0.044,    1.930,     0.6,   0.000,    0.000}, // 39
    {  487.249370,      23.500,      0.049,    1.920,     0.6,   0.000,    0.000}, // 40
    {  715.393150,       9.960,      0.145,    1.810,     0.6,   0.000,    0.000}, // 41
    {  773.839675,      67.100,      0.130,    1.820,     0.6,   0.000,    0.000}, // 42
    {  834.145330,      18.000,      0.147,    1.810 ,    0.6,   0.000,    0.000}}; // 43
  // number of lines of Liebe O2-line catalog (0-43 lines)
  const Index i_first = 0;
  const Index i_last  = 43; // all the spec. lines up to 1THz
  // const Index i_last  = 37; // only the 60GHz complex + 118GHz line
  

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the MPM87 model (Radio Science, 20(5), 1985, 1069):
  const Numeric CC_MPM93 = 1.00000;
  const Numeric CL_MPM93 = 1.00000;
  const Numeric CW_MPM93 = 1.00000;
  const Numeric CO_MPM93 = 1.00000;
  int   AppCutoff = 0;
  // ---------------------------------------------------------------------------------------


  // select the parameter set (!!model dominates values!!):
  Numeric CC, CL, CW, CO;
  if ( model == "MPM93" )
    {
      CC = CC_MPM93;
      CL = CL_MPM93;
      CW = CW_MPM93;
      CO = CO_MPM93;
    }
  else if ( model == "MPM93Lines" )
    {
      CC = 0.000;
      CL = CL_MPM93;
      CW = CW_MPM93;
      CO = CO_MPM93;
    }
  else if ( model == "MPM93Continuum" )
    {
      CC = CC_MPM93;
      CL = 0.000;
      CW = 0.000;
      CO = 0.000;
    }
  else if ( model == "MPM93NoCoupling" )
    {
      CC = CC_MPM93;
      CL = CL_MPM93;
      CW = CW_MPM93;
      CO = 0.000;
    }
  else if ( model == "MPM93NoCutoff" )
    {
      // !!ATTENTION!!
      // In the window regions the total absorption can get negative values.
      // So be carefull with this selection!
      CC = CC_MPM93;
      CL = CL_MPM93;
      CW = CW_MPM93;
      CO = CO_MPM93;
      AppCutoff = 1;
    }
  else if ( model == "user" )
    {
      CC = CCin;
      CL = CLin;
      CW = CWin;
      CO = COin;
    }
  else
    {
      ostringstream os;
      os << "O2-MPM93: ERROR! Wrong model values given.\n"
         << "Valid models are: 'MPM93' 'MPM93Lines' 'MPM93Continuum' 'MPM93NoCoupling' 'MPM93NoCutoff'" 
         << "and 'user'" << '\n';
      throw runtime_error(os.str());
    }
  out3  << "O2-MPM93: (model=" << model << ") parameter values in use:\n" 
        << " CC = " << CC << "\n"
        << " CL = " << CL << "\n"
        << " CW = " << CW << "\n"
        << " CO = " << CO << "\n";
  

  // const = VMR * ISORATIO = 0.20946 * 0.99519
  // this constant is already incorporated into the line strength, so we 
  // have top devide the line strength by this value since arts multiplies xsec
  // by these variables later in absCalc.
  const Numeric VMRISO = 0.2085;

  // O2 continuum parameters of MPM93:
  const Numeric S0 =  6.140e-5; // line strength                        [ppm]
  const Numeric G0 =  0.560e-3; // line width                           [GHz/hPa]
  const Numeric X0 =  0.800;    // temperature dependence of line width [1]

  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );

  // Loop pressure/temperature (pressure in hPa therefore the factor 0.01)
  for ( Index i=0; i<n_p; ++i )
    {
      // check if O2-VMR will cause an underflow due to division by zero:
      if (vmr[i] < VMRCalcLimit)
        {
          ostringstream os;
          os << "ERROR: MPM93 O2 full absorption model has detected a O2 volume mixing ratio of " 
             << vmr[i] << " which is below the threshold of " << VMRCalcLimit << ".\n"
             << "Therefore no calculation is performed.\n";
          throw runtime_error(os.str());
          return;
        }

      // relative inverse temperature [1]
      Numeric theta     = (300.0 / t_abs[i]);
      // H2O partial pressure [hPa]
      Numeric pwv       = Pa_to_hPa * p_abs[i] * h2o_abs[i];
      // dry air partial pressure [hPa]
      Numeric pda       = (Pa_to_hPa * p_abs[i]) - pwv;
      // here the total pressure is devided by the O2 vmr for the 
      // P_dry calculation because we calculate xsec and not abs: abs = vmr * xsec
      // old version without VMRISO: Numeric pda_dummy = pda / vmr[i];
      Numeric pda_dummy = pda;
      // O2 continuum strength [ppm]
      Numeric strength_cont =  S0 * pda_dummy * pow( theta, (Numeric)2. );
      // O2 continuum pseudo line broadening [GHz]
      Numeric gam_cont      =  G0 * (pwv+pda) *  pow( theta, X0 ); // GHz
      
      // Loop over input frequency
      for ( Index s=0; s<n_f; ++s )
        {
          // input frequency in [GHz]
          Numeric ff = f_mono[s] * Hz_to_GHz; 
          // O2 continuum absorption [1/m]
          // cross section: xsec = absorption / var
          // the vmr of O2 will be multiplied at the stage of absorption calculation:
          Numeric Nppc =  CC * strength_cont * ff * gam_cont /
                          ( pow( ff, (Numeric)2.)
                            + pow( gam_cont, (Numeric)2.) );
          
          // Loop over MPM93 O2 spectral lines:
          Numeric Nppl  = 0.0;
          for ( Index l = i_first; l <= i_last; ++l )
            {
              // line strength [ppm]   S=A(1,I)*P*V**3*EXP(A(2,I)*(1.-V))*1.E-6
              Numeric strength = CL * 1.000e-6  * pda_dummy * 
                                      mpm93[l][1] / mpm93[l][0] * 
                                      pow(theta, (Numeric)3.) * exp(mpm93[l][2]*(1.0-theta));
              // line broadening parameter [GHz]
              Numeric gam      = CW * ( mpm93[l][3] * 0.001 * 
                                      ( (       pda * pow(theta, ((Numeric)0.8-mpm93[l][4]))) + 
                                        (1.10 * pwv * theta) ) );
              // line mixing parameter [1]
              //                  if (l < 11) CD = 1.1000;
              Numeric delta    = CO * ( (mpm93[l][5] + mpm93[l][6] * theta) * 
                                      (pda+pwv) * pow(theta, (Numeric)0.8)
                                        * (Numeric)0.001 );
              // absorption [dB/km] like in the original MPM93
              Nppl            += strength * MPMLineShapeO2Function(gam, mpm93[l][0], ff, delta); 
            }
          // in MPM93 there is a cutoff for O2 line absorption if abs_l < 0 
          // absorption cannot be less than 0 according to MPM93 philosophy.
          if (AppCutoff == 0) 
            {
              if (Nppl < 0.000)  Nppl = 0.0000;// <---!!IMPORTANT FEATURE!!
            }
          //
          // O2 line absorption [1/m]
          // cross section: xsec = absorption / var
          // the vmr of O2 will be multiplied at the stage of absorption calculation:
          xsec(s,i) += dB_km_to_1_m * 0.1820 * ff * (Nppl+Nppc) / VMRISO;
        }
    }
  return;
}
//
// #################################################################################
// 
//   Oxygen complex at 60 GHz plus mm O2 lines plus O2 continuum
//
//    REFERENCES FOR EQUATIONS AND COEFFICIENTS:
//    P.W. Rosenkranz, CHAP. 2 and appendix, in ATMOSPHERIC REMOTE SENSING
//     BY MICROWAVE RADIOMETRY (M.A. Janssen, ed., 1993).
//    H.J. Liebe et al, JQSRT V.48, PP.629-643 (1992).
//    M.J. Schwartz, Ph.D. thesis, M.I.T. (1997).
//    SUBMILLIMETER LINE INTENSITIES FROM HITRAN96.
//    This version differs from Liebe's MPM92 in two significant respects:
//    1. It uses the modification of the 1- line width temperature dependence
//    recommended by Schwartz: (1/T).
//    2. It uses the same temperature dependence (X) for submillimeter 
//    line widths as in the 60 GHz band: (1/T)**0.8 
//
//   history:
//   05-01-95  P. Rosenkranz 
//   11-05-97  P. Rosenkranz - 1- line modification.
//   12-16-98  pwr - updated submm freq's and intensities from HITRAN96
//
void PWR93O2AbsModel( MatrixView        xsec,
                      const Numeric     CCin,      // model parameter
                      const Numeric     CLin,      // model parameter
                      const Numeric     CWin,      // model parameter
                      const Numeric     COin,      // model parameter
                      const String&     model,     // model selection string
                      const String&     version,   // PWR98, PWR93 or PWR88
                      ConstVectorView   f_mono,
                      ConstVectorView   p_abs,
                      ConstVectorView   t_abs,
                      ConstVectorView   vmrh2o,
                      ConstVectorView   vmr )
{
  const Index n_lines = 40; // all O2 lines in this model (range: 50-850 GHz)
  //
  // lines are arranged 1-,1+,3-,3+,etc. in spin-rotation spectrum
  // line center frequency in [GHz]
  const Numeric F93[n_lines] = { 118.7503,  56.2648,  62.4863,  58.4466,   // 00-03
                                  60.3061,  59.5910,  59.1642,  60.4348,   // 04-07
                                  58.3239,  61.1506,  57.6125,  61.8002,   // 08-11
                                  56.9682,  62.4112,  56.3634,  62.9980,   // 12-15
                                  55.7838,  63.5685,  55.2214,  64.1278,   // 16-19
                                  54.6712,  64.6789,  54.1300,  65.2241,   // 20-23
                                  53.5957,  65.7648,  53.0669,  66.3021,   // 24-27
                                  52.5424,  66.8368,  52.0214,  67.3696,   // 28-31
                                  51.5034,  67.9009, 368.4984, 424.7631,   // 32-35
                                 487.2494, 715.3932, 773.8397, 834.1453};  // 36-39

  // intensities in the submm range are updated according to HITRAN96
  const Numeric F98[n_lines] = { 118.7503,  56.2648,  62.4863,  58.4466,  60.3061,  59.5910,
                                  59.1642,  60.4348,  58.3239,  61.1506,  57.6125,  61.8002,
                                  56.9682,  62.4112,  56.3634,  62.9980,  55.7838,  63.5685,
                                  55.2214,  64.1278,  54.6712,  64.6789,  54.1300,  65.2241,
                                  53.5957,  65.7648,  53.0669,  66.3021,  52.5424,  66.8368,
                                  52.0214,  67.3696,  51.5034,  67.9009, 368.4984, 424.7632,
                                 487.2494, 715.3931, 773.8397, 834.1458};


  // line strength at T=300K in [cm² * Hz] 
  const Numeric S93[n_lines] = { 0.2936E-14, 0.8079E-15, 0.2480E-14, 0.2228E-14,
                                 0.3351E-14, 0.3292E-14, 0.3721E-14, 0.3891E-14,
                                 0.3640E-14, 0.4005E-14, 0.3227E-14, 0.3715E-14,
                                 0.2627E-14, 0.3156E-14, 0.1982E-14, 0.2477E-14,
                                 0.1391E-14, 0.1808E-14, 0.9124E-15, 0.1230E-14,
                                 0.5603E-15, 0.7842E-15, 0.3228E-15, 0.4689E-15,
                                 0.1748E-15, 0.2632E-15, 0.8898E-16, 0.1389E-15,
                                 0.4264E-16, 0.6899E-16, 0.1924E-16, 0.3229E-16,
                                 0.8191E-17, 0.1423E-16, 0.6460E-15, 0.7047E-14, 
                                 0.3011E-14, 0.1826E-14, 0.1152E-13, 0.3971E-14};

  // intensities in the submm range are updated according to HITRAN96
  const Numeric S98[n_lines] = { 0.2936E-14, 0.8079E-15, 0.2480E-14, 0.2228E-14,
                                 0.3351E-14, 0.3292E-14, 0.3721E-14, 0.3891E-14,
                                 0.3640E-14, 0.4005E-14, 0.3227E-14, 0.3715E-14,
                                 0.2627E-14, 0.3156E-14, 0.1982E-14, 0.2477E-14,
                                 0.1391E-14, 0.1808E-14, 0.9124E-15, 0.1230E-14,
                                 0.5603E-15, 0.7842E-15, 0.3228E-15, 0.4689E-15,
                                 0.1748E-15, 0.2632E-15, 0.8898E-16, 0.1389E-15,
                                 0.4264E-16, 0.6899E-16, 0.1924E-16, 0.3229E-16,
                                 0.8191E-17, 0.1423E-16, 0.6494E-15, 0.7083E-14, 
                                 0.3025E-14, 0.1835E-14, 0.1158E-13, 0.3993E-14};

  // temperature exponent of the line strength in [1]
  const Numeric BE[n_lines] = { 0.009,   0.015,   0.083,   0.084, 
                                0.212,   0.212,   0.391,   0.391, 
                                0.626,   0.626,   0.915,   0.915, 
                                1.260,   1.260,   1.660,   1.665,   
                                2.119,   2.115,   2.624,   2.625, 
                                3.194,   3.194,   3.814,   3.814, 
                                4.484,   4.484,   5.224,   5.224, 
                                6.004,   6.004,   6.844,   6.844, 
                                7.744,   7.744,   0.048,   0.044, 
                                0.049,   0.145,   0.141,   0.145};

  // widths in MHz/mbar for the O2 continuum
  const Numeric WB300 = 0.56; // [MHz/mbar]=[MHz/hPa]
  const Numeric X     = 0.80; // [1]

  // line width parameter [GHz/bar]
  const Numeric W300[n_lines] = {   1.630, 1.646, 1.468, 1.449, 
                                    1.382, 1.360, 1.319, 1.297, 
                                    1.266, 1.248, 1.221, 1.207, 
                                    1.181, 1.171, 1.144, 1.139, 
                                    1.110, 1.108, 1.079, 1.078, 
                                    1.050, 1.050, 1.020, 1.020, 
                                    1.000, 1.000, 0.970, 0.970,
                                    0.940, 0.940, 0.920, 0.920,
                                    0.890, 0.890, 1.920, 1.920, 
                                    1.920, 1.810, 1.810, 1.810};

  // y parameter for the calculation of Y [1/bar]
  const Numeric Y93[n_lines] = { -0.0233,  0.2408, -0.3486,  0.5227,
                                 -0.5430,  0.5877, -0.3970,  0.3237, 
                                 -0.1348,  0.0311,  0.0725, -0.1663, 
                                  0.2832, -0.3629,  0.3970, -0.4599,
                                  0.4695, -0.5199,  0.5187, -0.5597,
                                  0.5903, -0.6246,  0.6656, -0.6942,
                                  0.7086, -0.7325,  0.7348, -0.7546,
                                  0.7702, -0.7864,  0.8083, -0.8210,
                                  0.8439, -0.8529,  0.0000,  0.0000,
                                  0.0000,  0.0000,  0.0000,  0.0000};

  // y parameter for the calculation of Y [1/bar].
  // These values are from P. W. Rosenkranz, Interference coefficients for the 
  // overlapping oxygen lines in air, JQSRT, 1988, Volume 39, 287-297.
  const Numeric Y88[n_lines] = { -0.0244,  0.2772, -0.4068,  0.6270,
                                 -0.6183,  0.6766, -0.4119,  0.3290, 
                                  0.0317, -0.1591,  0.1145, -0.2068, 
                                  0.3398, -0.4158,  0.3922, -0.4482,
                                  0.4011, -0.4442,  0.4339, -0.4687,
                                  0.4783, -0.5074,  0.5157, -0.5403,
                                  0.5400, -0.5610,  0.5719, -0.5896,
                                  0.6046, -0.6194,  0.6347, -0.6468, 
                                  0.6627, -0.6718,  0.0000,  0.0000,
                                  0.0000,  0.0000,  0.0000,  0.0000};

  // v parameter for the calculation of Y [1/bar]
  const Numeric V[n_lines] ={    0.0079, -0.0978,  0.0844, -0.1273,
                                 0.0699, -0.0776,  0.2309, -0.2825, 
                                 0.0436, -0.0584,  0.6056, -0.6619, 
                                 0.6451, -0.6759,  0.6547, -0.6675,
                                 0.6135, -0.6139,  0.2952, -0.2895, 
                                 0.2654, -0.2590,  0.3750, -0.3680, 
                                 0.5085, -0.5002,  0.6206, -0.6091,
                                 0.6526, -0.6393,  0.6640, -0.6475,
                                 0.6729, -0.6545,  0.0000,  0.0000,
                                 0.0000,  0.0000,  0.0000,  0.0000};
  // range of lines to take into account for the line absorption part
  const Index first_line = 0;  // first line for calculation
  const Index last_line  = 39; // last line for calculation

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the Rosenkranz model 
  // (P. W. Rosenkranz, Chapter 2, pp 74, in M. A. Janssen, 
  // "Atmospheric Remote Sensing by Microwave Radiometry", John Wiley & Sons, Inc., 1993):
  const Numeric CC_PWR93 = 1.00000;
  const Numeric CL_PWR93 = 1.00000;
  const Numeric CW_PWR93 = 1.00000;
  const Numeric CO_PWR93 = 1.00000;
  // ---------------------------------------------------------------------------------------


  // select the parameter set (!!model dominates values!!):
  Numeric CC, CL, CW, CO, Y300[n_lines], S300[n_lines], F[n_lines];
  // FIXME int oldnewflag = 0;

  if ( model == "Rosenkranz" )
    {
      CC = CC_PWR93;
      CL = CL_PWR93;
      CW = CW_PWR93;
      CO = CO_PWR93;
    }
  else if ( model == "RosenkranzLines" )
    {
      CC = 0.000;
      CL = CL_PWR93;
      CW = CW_PWR93;
      CO = CO_PWR93;
    }
  else if ( model == "RosenkranzContinuum" )
    {
      CC = CC_PWR93;
      CL = 0.000;
      CW = 0.000;
      CO = 0.000;
    }
  else if ( model == "RosenkranzNoCoupling" )
    {
      CC = CC_PWR93;
      CL = CL_PWR93;
      CW = CW_PWR93;
      CO = 0.000;
    }
  else if ( model == "user" )
    {
      CC = CCin;
      CL = CLin;
      CW = CWin;
      CO = COin;
    }
  else
    {
      ostringstream os;
      os << "O2-PWR93: ERROR! Wrong model values given.\n"
         << "Valid models are: 'Rosenkranz', 'RosenkranzLines', RosenkranzContinuum, " 
         << "'RosenkranzNoCoupling', and 'user'" << '\n';
      throw runtime_error(os.str());
    }
  out3  << "O2-PWR93: (model=" << model << ") parameter values in use:\n" 
        << " CC = " << CC << "\n"
        << " CL = " << CL << "\n"
        << " CW = " << CW << "\n"
        << " CO = " << CO << "\n";
  

  // determin if version Rosenkranz 1993 or Rosenkranz 1988 is selected
  if ( (version != "PWR98") && (version != "PWR93") && (version != "PWR88") )
    {
      ostringstream os;
      os << "O2-PWR93/PWR88: ERROR! Wrong version is selected.\n"
         << "Valid versions are:\n" 
         << "  'PWR98'  updates of F and S to HISTRAN96 and M.J.Schwartz, MIT, 1997\n"
         << "           suggestions implemented.\n"
         << "  'PWR93'  for the oxygen absorption model described in  \n" 
         << "           P. W. Rosenkranz, Chapter 2, in M. A. Janssen,\n"
         << "           Atmospheric Remote Sensing by Microwave Radiometry,\n"
         << "           John Wiley & Sons, Inc., 1993.\n"
         << "  'PWR88'  for the oxygen absorption model described in \n" 
         << "           P. W. Rosenkranz, Interference coefficients for the \n" 
         << "           overlapping oxygen lines in air, \n"
         << "           JQSRT, 1988, Volume 39, 287-297.\n";
      throw runtime_error(os.str());
    }


  // select version dependent parameters
  if ( version == "PWR88" ) {
    for ( Index i=0; i<n_lines; ++i ) 
      {
        F[i]    = F93[i];
        S300[i] = S93[i];
        Y300[i] = Y88[i];
      };
  }
  if ( version == "PWR93" ) {
    for ( Index i=0; i<n_lines; ++i )
      {
        F[i]    = F93[i];
        S300[i] = S93[i];
        Y300[i] = Y93[i];
      };
  }
  if ( version == "PWR98" ) {
    for ( Index i=0; i<n_lines; ++i )
      {
        F[i]    = F98[i];
        S300[i] = S98[i];
        Y300[i] = Y93[i];
      };
  }

  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );
  
  // Loop pressure/temperature:
  for ( Index i=0; i<n_p; ++i )
    {
      // check if O2-VMR will cause an underflow due to division by zero:
      if (vmr[i] < VMRCalcLimit)
        {
          ostringstream os;
          os << "ERROR: PWR93 O2 full absorption model has detected a O2 volume mixing ratio of " 
             << vmr[i] << " which is below the threshold of " << VMRCalcLimit << ".\n"
             << "Therefore no calculation is performed.\n";
          throw runtime_error(os.str());
          return;
        }
      // relative inverse temperature [1]
      Numeric TH     = 3.0000e2 / t_abs[i];
      Numeric TH1    = (TH-1.000e0);
      Numeric B      = pow(TH, X);
      // partial pressure of H2O and dry air [hPa]
      Numeric PRESWV = Pa_to_hPa * (p_abs[i] * vmrh2o[i]);
      Numeric PRESDA = Pa_to_hPa * (p_abs[i] * (1.000e0 - vmrh2o[i]));
      Numeric DEN    = 0.001*(PRESDA*B + 1.1*PRESWV*TH); // [hPa]
      Numeric DENS   = 0.001*(PRESDA   + 1.1*PRESWV)*TH; // [hPa]
      Numeric DFNR   = WB300*DEN; // [GHz]
      
      // continuum absorption [1/m/GHz]
      Numeric CCONT  = CC * 1.23e-10 * pow( TH, (Numeric)2. ) * p_abs[i];

      // Loop over input frequency
      for ( Index s=0; s<n_f; ++s )
        {
          // initial O2 line absorption at position ff 
          // Numeric O2ABS  = 0.000e0;cd safff

          // input frequency in [GHz]
          Numeric ff   = Hz_to_GHz * f_mono[s]; 

          // continuum absorption [Neper/km]
          Numeric CONT = CCONT * (ff * ff * DFNR / (ff*ff + DFNR*DFNR));

          // Loop over Rosnekranz '93 spectral line frequency:
          Numeric SUM  = 0.000e0;
          for ( Index l=first_line; l<=last_line; ++l )
            {
              Numeric DF = CW * W300[l] * DEN; // [hPa]
              // 118 line update according to M. J. Schwartz, MIT, 1997
              if ( (version == "PWR98") && (fabs((F[l]-118.75)) < 0.10) )
                {
                  DF = CW * W300[l] * DENS; // [hPa]
                }
              Numeric Y    = CO * 0.001 * 0.01 * p_abs[i] * B * ( Y300[l] + V[l]*TH1 );
              Numeric STR  = CL * S300[l] * exp(-BE[l] * TH1);
              Numeric SF1  = ( DF + (ff-F[l])*Y ) / ( (ff-F[l])*(ff-F[l]) + DF*DF );
              Numeric SF2  = ( DF - (ff+F[l])*Y ) / ( (ff+F[l])*(ff+F[l]) + DF*DF );
              SUM         += STR * (SF1+SF2) * (ff/F[l]) * (ff/F[l]);
            }
          // O2 absorption [Neper/km]
          // Rosenkranz uses the factor 0.5034e12 in the calculation of the abs coeff.
          // This factor is the product of several terms:
          // 0.5034e12 = ISORATIO *   VMR   * (Hz/GHz) * (k_B*300K)^-1 
          //           = 0.995262 * 0.20946 *   10^-9  * 2.414322e21(hPa*cm^2*km)^-1
          //             |---- 0.2085 ----|   |---- 2.414322e12(hPa*cm^2*km)^-1 ---|
          //             |---- 0.2085 ----|   |---- 2.414322e10( Pa*cm^2*km)^-1 ---|
          // O2ABS = 2.4143e12 * SUM * PRESDA * pow(TH, 3.0) / PI;
          // O2ABS = CONT + (2.414322e10 * SUM * p_abs[i] * pow(TH, 3.0) / PI);
          // unit conversion x Nepers/km = y 1/m  --->  y = x * 1.000e-3 
          // therefore 2.414322e10 --> 2.414322e7
          // xsec [1/m] 
          xsec(s,i) += CONT + (2.414322e7 * SUM * p_abs[i] * pow(TH, (Numeric)3.) / PI);
        }
    }
  return;
}
//
// #################################################################################
//
// MPM93 O2 continuum:
// see publication side of National Telecommunications and Information Administration
//   http://www.its.bldrdoc.gov/pub/all_pubs/all_pubs.html
// and ftp side for downloading the MPM93 original source code:
//   ftp://ftp.its.bldrdoc.gov/pub/mpm93/
void MPM93_O2_continuum( MatrixView          xsec,
                         const Numeric       S0in,         // model parameter
                         const Numeric       G0in,         // model parameter
                         const Numeric       XS0in,        // model parameter
                         const Numeric       XG0in,        // model parameter
                         const String&       model,
                         ConstVectorView     f_mono,
                         ConstVectorView     p_abs,
                         ConstVectorView     t_abs,
                         ConstVectorView     h2o_abs,
                         ConstVectorView     vmr         )
{

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the MPM93 model (J. Liebe and G. A. Hufford and M. G. Cotton,
  // "Propagation modeling of moist air and suspended water/ice
  // particles at frequencies below 1000 GHz",
  // AGARD 52nd Specialists Meeting of the Electromagnetic Wave
  // Propagation Panel, Palma de Mallorca, Spain, 1993, May 17-21):
  // const Numeric      S0_MPM93  =  6.140e-13/0.20946; // line strength/VMR-O2 [1/Pa] 
  const Numeric S0_MPM93  =  6.140e-13;         // line strength [1/Pa] 
  const Numeric G0_MPM93  =  0.560e4;           // line width [Hz/Pa]
  const Numeric XS0_MPM93 =  2.000;             // temperature dependence of line strength
  const Numeric XG0_MPM93 =  0.800;             // temperature dependence of line width
  // ---------------------------------------------------------------------------------------


  // select the parameter set (!!model dominates parameters!!):
  Numeric S0, G0, XS0, XG0;
  if ( model == "MPM93" )
    {
      S0  = S0_MPM93;
      G0  = G0_MPM93;
      XS0 = XS0_MPM93;
      XG0 = XG0_MPM93;
    }
  else if ( model == "user" )
    {
      S0  = S0in;
      G0  = G0in;
      XS0 = XS0in;
      XG0 = XG0in;
    }
  else
    {
      ostringstream os;
      os << "O2-SelfContMPM93: ERROR! Wrong model values given.\n"
         << "Valid models are: 'MPM93' and 'user'" << '\n';
      throw runtime_error(os.str());
    }
  out3  << "O2-SelfContMPM93: (model=" << model << ") parameter values in use:\n" 
        << " S0  = " << S0 <<  "\n"
        << " G0  = " << G0 <<  "\n"
        << " XS0 = " << XS0 << "\n"
        << " XG0 = " << XG0 << "\n";
  
  
  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );

  // const = VMR * ISORATIO = 0.20946 * 0.99519
  // this constant is already incorporated into the line strength, so we 
  // have top devide the line strength by this value since arts multiplies xsec
  // by these variables later in absCalc.
  const Numeric VMRISO = 0.2085;
  

  // Loop pressure/temperature:
  for ( Index i=0; i<n_p; ++i )
    {
      if (vmr[i] < VMRCalcLimit) // make sure that division by zero is excluded
        {
          ostringstream os;
          os << "ERROR: MPM93 O2 continuum absorption model has detected a O2 volume mixing ratio of " 
             << vmr[i] << " which is below the threshold of " << VMRCalcLimit << ".\n"
             << "Therefore no calculation is performed.\n";
          throw runtime_error(os.str());
          return;
        }
      Numeric th       = 300.0 / t_abs[i]; // Theta
      // continuum strength
      Numeric strength =  S0 * p_abs[i] * (1.0000 - h2o_abs[i]) * pow( th, XS0 );
      // G0 from the input has to be converted to unit GHz/hPa --> * 1.0e-7
      Numeric gamma    =  G0 * p_abs[i] * pow( th, XG0 ); // Hz
          
      // Loop frequency:
      for ( Index s=0; s<n_f; ++s )
        {
          // the vmr of O2 will be multiplied at the stage of absorption calculation:
          // abs / vmr * xsec.
          xsec(s,i) +=  (4.0 * PI / SPEED_OF_LIGHT)  *              // unit factor [1/(m*Hz)] 
                        (strength / VMRISO)          *              // strength    [1]
                        ( pow( f_mono[s], (Numeric)2.) * gamma /              // line shape  [Hz]
                          ( pow( f_mono[s], (Numeric)2.) + pow( gamma, (Numeric)2.) ) );
        }
    }
  return;
}
//
// #################################################################################
//
//   3) O2-air : P. W. Rosenkranz Chapter 2, pp 74, in M. A. Janssen, 
//               "Atmospheric Remote Sensing by Microwave Radiometry",
//               John Wiley & Sons, Inc., 1993. Also stated in 
//               Liebe et al. JQSRT, Vol 48, Nr 5/6, pp. 629-643, 1992.
//               Default continuum parameters are  C=1.6E-17*10E-9,  x=0.8
void Rosenkranz_O2_continuum( MatrixView        xsec,
                              const Numeric     S0in,         // model parameter
                              const Numeric     G0in,         // model parameter
                              const Numeric     XS0in,        // model parameter
                              const Numeric     XG0in,        // model parameter
                              const String&     model,
                              ConstVectorView   f_mono,
                              ConstVectorView   p_abs,        // total pressure [Pa]
                              ConstVectorView   t_abs,
                              ConstVectorView   h2o_abs,      // H2O VMR
                              ConstVectorView   vmr      )    // O2 VMR
{

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // P. W. Rosenkranz, Chapter 2, in M. A. Janssen,
  // Atmospheric Remote Sensing by Microwave Radiometry, John Wiley & Sons, Inc., 1993
  // ftp://mesa.mit.edu/phil/lbl_rt
  const Numeric S0_PWR93   =  1.11e-14; // [K²/(Hz*Pa*m)] line strength
  const Numeric G0_PWR93  =  5600.000;  // line width [Hz/Pa]
  const Numeric XS0_PWR93 =  2.000;    // temperature dependence of line strength
  const Numeric XG0_PWR93 =  0.800;    // temperature dependence of line width
  // ---------------------------------------------------------------------------------------

  // select the parameter set (!!model dominates values!!):
  Numeric S0, G0, XS0, XG0;
  if ( model == "Rosenkranz" )
    {
      S0  = S0_PWR93;
      G0  = G0_PWR93;
      XS0 = XS0_PWR93;
      XG0 = XG0_PWR93;
    }
  else if ( model == "user" )
    {
      S0  = S0in;
      G0  = G0in;
      XS0 = XS0in;
      XG0 = XG0in;
    }
  else
    {
      ostringstream os;
      os << "O2-SelfContPWR93: ERROR! Wrong model values given.\n"
         << "Valid models are: 'Rosenkranz' and 'user'" << '\n';
      throw runtime_error(os.str());
    }
  out3  << "O2-SelfContPWR93: (model=" << model << ") parameter values in use:\n" 
        << " S0  = " << S0 <<  "\n"
        << " G0  = " << G0 <<  "\n"
        << " XS0 = " << XS0 << "\n"
        << " XG0 = " << XG0 << "\n";
  

  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );

  // loop over all pressure levels:
  for ( Index i=0; i<n_p; ++i )
    {
      Numeric TH = 300.00 / t_abs[i];         // relative temperature  [1]
      
      Numeric ph2o  = p_abs[i] * h2o_abs[i];  // water vapor partial pressure [Pa]
      Numeric pdry  = p_abs[i] - ph2o;        // dry air partial pressure     [Pa]


      // pseudo broadening term [Hz]
      Numeric gamma = G0 * (pdry * pow( TH, XG0 ) + 1.100 * ph2o * TH); 

      // Loop over frequency grid:
      for ( Index s=0; s<n_f; ++s )
        {
          // division by vmr of O2 is necessary because of the absorption calculation
          // abs = vmr * xsec.
          xsec(s,i) += S0 * p_abs[i] / pow( t_abs[i], XS0 ) * 
                        ( pow( f_mono[s], (Numeric)2. )
                          * gamma / ( pow( f_mono[s], 2 )
                                      + pow( gamma, (Numeric)2. ) ) ) ;
        }
    }
}
//
//
// #################################################################################
//
void Standard_O2_continuum( MatrixView        xsec,         // cross section
                            const Numeric     Cin,          // model parameter
                            const Numeric     G0in,         // model parameter
                            const Numeric     G0Ain,        // model parameter
                            const Numeric     G0Bin,        // model parameter
                            const Numeric     XG0din,       // model parameter
                            const Numeric     XG0win,       // model parameter
                            const String&     model,        // model parameter
                            ConstVectorView   f_mono,       // frequency grid
                            ConstVectorView   p_abs,        // P_tot grid
                            ConstVectorView   t_abs,        // T grid
                            ConstVectorView   h2o_abs,      // VMR H2O profile
                            ConstVectorView   vmr       )   // VMR O2  profile
{

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // P. W. Rosenkranz, Chapter 2, in M. A. Janssen,
  // Atmospheric Remote Sensing by Microwave Radiometry, John Wiley & Sons, Inc., 1993
  // ftp://mesa.mit.edu/phil/lbl_rt
  const Numeric C_PWR93    = (1.108e-14/pow((Numeric)3.0e2,(Numeric)2.)); // [1/(Hz*Pa*m)] line strength
  const Numeric G0_PWR93   = 5600.000;  // line width [Hz/Pa]
  const Numeric G0A_PWR93  =    1.000;  // line width [1]
  const Numeric G0B_PWR93  =    1.100;  // line width [1]
  const Numeric XG0d_PWR93 =    0.800;  // temperature dependence of line width [1]
  const Numeric XG0w_PWR93 =    1.000;  // temperature dependence of line width [1]
  //
  // standard values for the MPM93 model (J. Liebe and G. A. Hufford and M. G. Cotton,
  // "Propagation modeling of moist air and suspended water/ice
  // particles at frequencies below 1000 GHz",
  // AGARD 52nd Specialists Meeting of the Electromagnetic Wave
  // Propagation Panel, Palma de Mallorca, Spain, 1993, May 17-21):
  // const Numeric      C_MPM93    = 1.23e-19; // line strength/VMR [1/m*1/Hz*1/Pa] 
  const Numeric C_MPM93    = 6.14e-13*(4.0*PI/SPEED_OF_LIGHT)/0.2085; // line strength [1/m*1/Hz*1/Pa]
  // 0.2085 = VMR * ISORATIO = 0.20946 * 0.99519
  const Numeric G0_MPM93   = 5600.000; // line width [Hz/Pa]
  const Numeric G0A_MPM93  =    1.000; // line width [1]
  const Numeric G0B_MPM93  =    1.000; // line width [1]
  const Numeric XG0d_MPM93 =    0.800; // temperature dependence of line strength [1]
  const Numeric XG0w_MPM93 =    0.800; // temperature dependence of line width    [1]
  // ---------------------------------------------------------------------------------------

  // select the parameter set (!!model dominates values!!):
  Numeric C, G0, G0A, G0B, XG0d, XG0w;
  if ( model == "Rosenkranz" )
    {
      C    = C_PWR93;
      G0   = G0_PWR93;
      G0A  = G0A_PWR93;
      G0B  = G0B_PWR93;
      XG0d = XG0d_PWR93;
      XG0w = XG0w_PWR93;
    }
  else if ( model == "MPM93" )
    {
      C    = C_MPM93;
      G0   = G0_MPM93;
      G0A  = G0A_MPM93;
      G0B  = G0B_MPM93;
      XG0d = XG0d_MPM93;
      XG0w = XG0w_MPM93;
    }
  else if ( model == "user" )
    {
      C    = Cin;
      G0   = G0in;
      G0A  = G0Ain;
      G0B  = G0Bin;
      XG0d = XG0din;
      XG0w = XG0win;
    }
  else
    {
      ostringstream os;
      os << "O2-GenerealCont: ERROR! Wrong model values given.\n"
         << "Valid models are: 'Rosenkranz', 'MPM93' and 'user'" << '\n';
      throw runtime_error(os.str());
    }
  out3  << "O2-GeneralCont: (model=" << model << ") parameter values in use:\n" 
        << " C    = " << C <<  "\n"
        << " G0   = " << G0 <<  "\n"
        << " G0A  = " << G0A <<  "\n"
        << " G0B  = " << G0B <<  "\n"
        << " XG0d = " << XG0d << "\n"
        << " XG0w = " << XG0w << "\n";
  

  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );

  // const = VMR * ISORATIO = 0.20946 * 0.99519
  // this constant is already incorporated into the line strength, so we 
  // have top devide the line strength by this value since arts multiplies xsec
  // by these variables later in absCalc.
  // FIXME const Numeric        VMRISO = 0.2085;

  // loop over all pressure levels:
  for ( Index i=0; i<n_p; ++i )
    {
      Numeric TH = 3.0e2 / t_abs[i];         // relative temperature  [1]
      
      Numeric ph2o = p_abs[i] * h2o_abs[i];  // water vapor partial pressure [Pa]
      Numeric pdry = p_abs[i] - ph2o;        // dry air partial pressure     [Pa]


      // pseudo broadening term [Hz]
      Numeric gamma = G0 * (G0A * pdry * pow( TH, XG0d ) + G0B * ph2o * pow( TH, XG0w )); 

      // Loop over frequency grid:
      for ( Index s=0; s<n_f; ++s )
        {
          // division by vmr of O2 is necessary because of the absorption calculation
          // abs = vmr * xsec.
          xsec(s,i) += C * p_abs[i] * pow( TH, (Numeric)2. ) * 
                       ( gamma * pow( f_mono[s], (Numeric)2. ) / 
                         ( pow( f_mono[s], 2 ) + pow( gamma, (Numeric)2. ) ) );
        }
    }
}
//
// #################################################################################
// ################################ NITROGEN MODELS ################################
// #################################################################################
//
// Borysow-Frommhold 1986 N2-N2 CIA absorption model;
// see publication A. Borysow and L. Frommhold, 
//                 The Astrophysical Journal, vol.311, pp.1043-1057, 1986
//                 see http://adsabs.harvard.edu/article_service.html for a scanned 
//                 version of the paper
void BF86_CIA_N2( MatrixView          xsec,
                  const Numeric       Cin,
                  const String&       model,
                  ConstVectorView     f_mono,
                  ConstVectorView     p_abs,
                  ConstVectorView     t_abs,
                  ConstVectorView     vmr   )
{
  //
  //
  // external function to call (original F77 code translated with f2c)
  extern Numeric n2n2tks_(double t, double f);
  //
  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the MPM93 H2O continuum model 
  // (AGARD 52nd Specialists Meeting of the Electromagnetic Wave
  // Propagation Panel, Palma de Mallorca, Spain, 1993, May 17-21):
  Numeric  XFAC  =  1.0000;             // scaling factor
  // ---------------------------------------------------------------------------------------
  
  // select the parameter set (!!model dominates values!!):
  if ( model == "BF86" )
    {
      XFAC =  1.0000;
    }
  else if ( model == "user" )
    {
      XFAC =  Cin;
    }
  else
    {
      ostringstream os;
      os << "N2-SelfContBorysow: ERROR! Wrong model values given.\n"
         << "allowed models are: 'BF86', 'user'" << '\n';
      throw runtime_error(os.str());
    }
  
  out3  << "N2-SelfContBorysow: (model=" << model << ") parameter values in use:\n" 
        << " XFAC = " << XFAC << "\n";
  
  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies


  const Numeric AMAG2DEN = 44.53807; // inverse of N2 mol volume at std p/T
  const Numeric RIDGAS =  8.314510;  // ideal gas constant

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );
  
  // Loop pressure/temperature:
  for ( Index i=0; i<n_p; ++i )
    {
      //cout << "------------------------------------------------\n";
      double T = (double) t_abs[i];
      //cout << "N2-N2 BF86: T     =" << T << " K\n";
      //cout << "N2-N2 BF86: p     =" << p_abs[i] << " Pa\n";
      //cout << "N2-N2 BF86: VMR   =" << vmr[i] << "\n";
      Numeric XAMA  = (p_abs[i]) / ( AMAG2DEN * RIDGAS * t_abs[i] );
      Numeric XAMA2 = pow(XAMA,(Numeric)2.);
      //cout << "N2-N2 BF86: XAMA  =" << XAMA << "\n";

      // Loop frequency:
      for ( Index s=0; s<n_f; ++s )
        {
          // the second vmr of N2 will be multiplied at the stage of
          // absorption calculation: abs =  vmr * xsec.
          double f = (double) f_mono[s];
          //cout << "N2-N2 BF86: f     =" << f << " Hz\n";
          double cont = n2n2tks_(T, f);
          xsec(s,i) += (Numeric) (cont * 1.000e2 * vmr[i] * XAMA2);
          //cout << "N2-N2 BF86: cont  =" << cont << " cm-1 * amagat-2\n";
          //cout << "N2-N2 BF86: abs   =" << (vmr[i] * xsec(s,i)) << " m-1\n";
        }
    }
  return;
}
//
// #################################################################################
//
// MPM93 N2 continuum:
// see publication side of National Telecommunications and Information Administration
//   http://www.its.bldrdoc.gov/pub/all_pubs/all_pubs.html
// and ftp side for downloading the MPM93 original source code:
//   ftp://ftp.its.bldrdoc.gov/pub/mpm93/
void MPM93_N2_continuum( MatrixView          xsec,
                         const Numeric       Cin,
                         const Numeric       Gin,
                         const Numeric       xTin,
                         const Numeric       xfin,
                         const String&       model,
                         ConstVectorView     f_mono,
                         ConstVectorView     p_abs,
                         ConstVectorView     t_abs,
                         ConstVectorView     h2o_abs,
                         ConstVectorView     vmr         )
{

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the MPM93 H2O continuum model 
  // (AGARD 52nd Specialists Meeting of the Electromagnetic Wave
  // Propagation Panel, Palma de Mallorca, Spain, 1993, May 17-21):
  const Numeric xT_MPM93  =  3.500;             // temperature exponent [1]
  const Numeric xf_MPM93  =  1.500;             // frequency exponent [1]
  const Numeric gxf_MPM93 =  9.000*xf_MPM93;    // needed for the unit conversion of G_MPM93
  const Numeric S_MPM93   =  2.296e-31;         // line strength  [1/Pa² * 1/Hz]
  const Numeric G_MPM93   =  1.930e-5*pow((Numeric)10.000, -gxf_MPM93); // frequency factor [1/Hz^xf]
  // ---------------------------------------------------------------------------------------
  
  // select the parameter set (!!model dominates values!!):
  Numeric S0, G0, xf, xT, gxf;
  if ( model == "MPM93" )
    {
      S0  = S_MPM93;
      G0  = G_MPM93;
      xT  = xT_MPM93;
      xf  = xf_MPM93;
      gxf = gxf_MPM93;
    }
  else if ( model == "MPM93Scale" )
    {
      S0  = Cin * S_MPM93;
      G0  = G_MPM93;
      xT  = xT_MPM93;
      xf  = xf_MPM93;
      gxf = gxf_MPM93;
    }
  else if ( model == "user" )
    {
      S0  = Cin;
      G0  = Gin;
      xT  = xTin;
      xf  = xfin;
      gxf = 9.000*xf;
    }
  else
    {
      ostringstream os;
      os << "N2-SelfContMPM93 : ERROR! Wrong model values given.\n"
         << "allowed models are: 'MPM93', 'MPM93Scale' or 'user'" << '\n';
      throw runtime_error(os.str());
    }
  
  out3  << "N2-SelfContMPM93: (model=" << model << ") parameter values in use:\n" 
        << " S0 = " << S0 << "\n"
        << " G0 = " << G0 << "\n"
        << " xT = " << xT << "\n"
        << " xf = " << xf << "\n";
  
  // unit conversion internally:
  //const Numeric S0unitconv = 1.000e+13;  // x [1/(hPa²*GHz)] => y [1/(pa²*Hz)]
  //const Numeric G0unitconv = pow(10.000, gxf);

  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );
  
  Numeric fac = 4.0 * PI / SPEED_OF_LIGHT;  //  = 4 * pi / c
  // Loop pressure/temperature:
  for ( Index i=0; i<n_p; ++i )
    {
      Numeric th = 300.0 / t_abs[i];
      Numeric strength =  S0 * 
                          pow( (p_abs[i] * ((Numeric)1.0000 - h2o_abs[i])),
                               (Numeric)2. )
                          * pow( th, xT );

      // Loop frequency:
      for ( Index s=0; s<n_f; ++s )
        {
          // FIXME Numeric f = f_mono[s] * Hz_to_GHz; // frequency in GHz
          // the vmr of N2 will be multiplied at the stage of absorption calculation:
          // abs / vmr * xsec.
          xsec(s,i) += fac * strength *                              // strength
                       pow(f_mono[s], (Numeric)2.) /                      // frequency dependence
                       ( 1.000 + G0 * pow( f_mono[s], xf) ) *  
                        vmr[i];                                // N2 vmr
        }
    }
  return;
}
//
// #################################################################################
//
void Pardo_ATM_N2_dry_continuum( MatrixView          xsec,
                                 const Numeric       Cin,
                                 const String&       model,
                                 ConstVectorView     f_mono,
                                 ConstVectorView     p_abs,
                                 ConstVectorView     t_abs,
                                 ConstVectorView     vmr,
                                 ConstVectorView     h2ovmr      )
{
  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the Pardo et al. model (IEEE, Trans. Ant. Prop., 
  // Vol 49, No 12, pp. 1683-1694, 2001)
  const Numeric C_ATM = 2.612e-6; // [1/m]
  // ---------------------------------------------------------------------------------------

  // select the parameter set (!!model dominates parameters!!):
  Numeric C;
   if ( model == "ATM" )
     {
       C = C_ATM;
     }
   else if ( model == "user" )
     {
       C = Cin;
     }
   else
     {
       ostringstream os;
       os << "N2-DryContATM01: ERROR! Wrong model values given.\n"
          << "allowed models are: 'ATM', 'user'" << '\n';
       throw runtime_error(os.str());
     }
   out3  << "N2-DryContATM01: (model=" << model << ") parameter values in use:\n" 
         << " C_s = " << C << "\n";

   const Index n_p = p_abs.nelem();     // Number of pressure levels
   const Index n_f = f_mono.nelem();    // Number of frequencies

   // Check that dimensions of p_abs, t_abs, and vmr agree:
   assert ( n_p==t_abs.nelem() );
   assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );
  
  // Loop over pressure/temperature grid:
  for ( Index i=0; i<n_p; ++i )
    {
      // since this is an effective "dry air" continuum, it is not really
      // it is not specifically attributed to N2, so we need the total 
      // dry air part in total which is equal to the total minus the 
      // water vapor pressure:
      Numeric  pd = p_abs[i] * ( 1.00000e0 - h2ovmr[i] ); // [Pa]
      // Loop over frequency grid:
      if (vmr[i] > VMRCalcLimit )
        {
          for ( Index s=0; s<n_f; ++s )
            {
              // Becaue this is an effective "dry air" continuum, it is not really
              // specific N2 but mainly caused by N2. Therefore the N2 vmr must be 
              // canceled out here which is later in absCalc multiplied 
              // (calculation: abs = vmr * xsec):
              xsec(s,i) += C *                    // strength [1/(m*Hz²Pa²)] 
                pow( (f_mono[s]/(Numeric)2.25e11), (Numeric)2. ) * // quadratic f dependence [Hz²]
                pow( ((Numeric)300.0/t_abs[i]), (Numeric)3.5 )   * // free T dependence      [1]
                pow( (pd/(Numeric)1.01300e5), (Numeric)2. )      / // quadratic p dependence [Pa²]
                vmr[i];                                            // cancel the vmr dependency
            }
        }
    }
}
//
// #################################################################################
//
void Rosenkranz_N2_self_continuum( MatrixView          xsec,
                                   const Numeric       Cin,
                                   const Numeric       xin,
                                   const String&       model,
                                   ConstVectorView     f_mono,
                                   ConstVectorView     p_abs,
                                   ConstVectorView     t_abs,
                                   ConstVectorView     vmr       )
{
  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the Rosenkranz model (Chapter 2, pp 74, in M. A. Janssen, 
  // "Atmospheric Remote Sensing by Microwave Radiometry", John Wiley & Sons, Inc., 1993
  const Numeric C_PWR = 1.05e-38; // [1/(Pa²*Hz²*m)]
  const Numeric x_PWR = 3.55;     // [1]
  // ---------------------------------------------------------------------------------------

  // select the parameter set (!!model dominates parameters!!):
  Numeric C, x;
   if ( model == "Rosenkranz" )
     {
       C = C_PWR;
       x = x_PWR;
     }
   else if ( model == "user" )
     {
       C = Cin;
       x = xin;
     }
   else
     {
       ostringstream os;
       os << "N2-SelfContPWR93: ERROR! Wrong model values given.\n"
          << "allowed models are: 'Rosenkranz', 'user'" << '\n';
       throw runtime_error(os.str());
     }
   out3  << "N2-SelfContPWR93: (model=" << model << ") parameter values in use:\n" 
         << " C_s = " << C << "\n"
         << " x_s = " << x << "\n";

   const Index n_p = p_abs.nelem();     // Number of pressure levels
   const Index n_f = f_mono.nelem();    // Number of frequencies

   // Check that dimensions of p_abs, t_abs, and vmr agree:
   assert ( n_p==t_abs.nelem() );
   assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );
  
  // Loop over pressure/temperature grid:
  for ( Index i=0; i<n_p; ++i )
    {
      // Loop over frequency grid:
      for ( Index s=0; s<n_f; ++s )
        {
          // The second vmr of N2 will be multiplied at the stage of absorption 
          // calculation: abs = vmr * xsec.
          xsec(s,i) += C *                        // strength [1/(m*Hz²Pa²)] 
                       pow( f_mono[s], (Numeric)2. ) *      // quadratic f dependence [Hz²]
                       pow( (Numeric)300.0/t_abs[i], x ) * // free T dependence      [1]
                       pow( p_abs[i], (Numeric)2. ) *       // quadratic p dependence [Pa²]
                       vmr[i];                    // second N2-VMR at the stage 
                                                  // of absorption calculation
        }
    }
}
//
// #################################################################################
//
// 4) N2-N2  : P. W. Rosenkranz Chapter 2, pp 74, in M. A. Janssen, 
//    "Atmospheric Remote Sensing by Microwave Radiometry", John Wiley & Sons, Inc., 1993
//
void Standard_N2_self_continuum( MatrixView          xsec,
                                 const Numeric       Cin,
                                 const Numeric       xfin,
                                 const Numeric       xtin,
                                 const Numeric       xpin,
                                 const String&       model,
                                 ConstVectorView     f_mono,
                                 ConstVectorView     p_abs,
                                 ConstVectorView     t_abs,
                                 ConstVectorView     vmr         )
{

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the Rosenkranz model, Chapter 2, pp 74, in M. A. Janssen, 
  // "Atmospheric Remote Sensing by Microwave Radiometry", John Wiley & Sons, Inc., 1993
  const Numeric C_GM  = 1.05e-38; // [1/(Pa²*Hz²*m)]
  const Numeric xf_GM = 2.00;     // [1]
  const Numeric xt_GM = 3.55;     // [1]
  const Numeric xp_GM = 2.00;     // [1]
  // ---------------------------------------------------------------------------------------

  // select the parameter set (!!model dominates over values!!):
  Numeric C, xt, xf, xp;
   if ( model == "Rosenkranz" )
     {
       C  = C_GM;
       xt = xt_GM;
       xf = xf_GM;
       xp = xp_GM;
     }
   else if ( model == "user" )
     {
       C  = Cin;
       xt = xtin;
       xf = xfin;
       xp = xpin;
     }
   else
     {
       ostringstream os;
       os << "N2-SelfContStandardType: ERROR! Wrong model values given.\n"
          << "allowed models are: 'Rosenkranz', 'user'" << '\n';
       throw runtime_error(os.str());
     }
   out3  << "N2-SelfContStandardType: (model=" << model << ") parameter values in use:\n" 
         << " C  = " << C  << "\n"
         << " xt = " << xt << "\n"
         << " xf = " << xf << "\n"
         << " xp = " << xp << "\n";


  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );
  
  // Loop over pressure/temperature grid:
  for ( Index i=0; i<n_p; ++i )
    {
      //cout << "vmr[" << i << "]= " << vmr[i] << "\n";
      // Loop over frequency grid:
      for ( Index s=0; s<n_f; ++s )
        {
          // The second N2-VMR will be multiplied at the stage of absorption 
          // calculation: abs = vmr * xsec.
          xsec(s,i) += C                            * // strength [1/(m*Hz²Pa²)]  
                       pow( ((Numeric)300.00/t_abs[i]), xt ) * // T dependence        [1] 
                       pow( f_mono[s], xf )         * // f dependence    [Hz^xt]  
                       pow( p_abs[i], xp )          * // p dependence    [Pa^xp]
                       pow( vmr[i], (xp-(Numeric)1.) );         // last N2-VMR at the stage 
                                                      // of absorption calculation
        }
    }
}
//
// #################################################################################
// ############################## CARBON DIOXIDE MODELS ############################
// #################################################################################
//
void Rosenkranz_CO2_self_continuum( MatrixView          xsec,
                                    const Numeric       Cin,
                                    const Numeric       xin,
                                    const String&       model,
                                    ConstVectorView     f_mono,
                                    ConstVectorView     p_abs,
                                    ConstVectorView     t_abs,
                                    ConstVectorView     vmr      )
{
  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // P. W. Rosenkranz Chapter 2, pp 74, in M. A. Janssen, 
  // "Atmospheric Remote Sensing by Microwave Radiometry", John Wiley & Sons, Inc., 1993
  const Numeric C_PWR = 7.43e-37; // [ 1/(Pa²*Hz²*m) ]
  const Numeric x_PWR = 5.08;     // [ 1 ]
  // ---------------------------------------------------------------------------------------

  // select the parameter set (!!model dominates values!!):
  Numeric C, x;
  if ( model == "Rosenkranz" )
    {
      C = C_PWR;
      x = x_PWR;
    }
  else if ( model == "user" )
    {
      C = Cin;
      x = xin;
    }
  else
    {
      ostringstream os;
      os << "CO2-SelfContPWR93 : ERROR! Wrong model values given.\n"
         << "allowed models are: 'Rosenkranz', 'user'" << "\n";
      throw runtime_error(os.str());
    }
  
  out3  << "CO2-SelfContPWR93: (model=" << model << ") parameter values in use:\n" 
        << " C = " << C << "\n"
        << " x = " << x << "\n";

  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );
  
  // Loop over pressure/temperature grid:
  for ( Index i=0; i<n_p; ++i )
    {
      // Dummy scalar holds everything except the quadratic frequency dependence.
      // The second vmr of CO2 will be multiplied at the stage of absorption 
      // calculation: abs = vmr * xsec.
      Numeric dummy =
        C * pow( (Numeric)300./t_abs[i], x ) * pow( p_abs[i], (Numeric)2. ) * vmr[i];

      // Loop over frequency grid:
      for ( Index s=0; s<n_f; ++s )
        {
          xsec(s,i) += dummy * pow( f_mono[s], (Numeric)2. );
        }
    }
}
//
// #################################################################################
//
void Rosenkranz_CO2_foreign_continuum( MatrixView          xsec,
                                       const Numeric       Cin,
                                       const Numeric       xin,
                                       const String&       model,
                                       ConstVectorView     f_mono,
                                       ConstVectorView     p_abs,
                                       ConstVectorView     t_abs,
                                       ConstVectorView     n2_abs,
                                       ConstVectorView     vmr   )
{

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // "Atmospheric Remote Sensing by Microwave Radiometry", John Wiley & Sons, Inc., 1993
  const Numeric C_PWR = 2.71e-37; // default: 2.71*10^-37 1/(Pa²*Hz²*m)
  const Numeric x_PWR = 4.7;      // default: 4.7
  // ---------------------------------------------------------------------------------------

  // select the parameter set (!!model dominates values!!):
  Numeric C, x;
  if ( model == "Rosenkranz" )
    {
      C = C_PWR;
      x = x_PWR;
    }
  else if ( model == "user" )
    {
      C = Cin;
      x = xin;
    }
  else
    {
      ostringstream os;
      os << "CO2-ForeignContPWR93: ERROR! Wrong model values given.\n"
         << "allowed models are: 'Rosenkranz', 'user'" << "\n";
      throw runtime_error(os.str());
    }
  
  out3  << "CO2-ForeignContPWR93: (model=" << model << ") parameter values in use:\n" 
        << " C = " << C << "\n"
        << " x = " << x << "\n";

  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );
  
  // Loop pressure/temperature:
  for ( Index i=0; i<n_p; ++i )
    {
      // Dummy scalar holds everything except the quadratic frequency dependence.
      // The vmr of CO2 will be multiplied at the stage of absorption 
      // calculation: abs = vmr * xsec.
      Numeric dummy = C * pow( (Numeric)300./t_abs[i], x ) * p_abs[i] * p_abs[i] * n2_abs[i];

      // Loop frequency:
      for ( Index s=0; s<n_f; ++s )
        {
          xsec(s,i) += dummy * pow( f_mono[s], (Numeric)2. );
        }
    }
}
//
// #################################################################################
// ################################### CLOUD AND RAIN MODELS #######################
// #################################################################################
//
void MPM93WaterDropletAbs( MatrixView         xsec,
                           const Numeric      CCin,   // input parameter
                           const Numeric      CGin,   // input parameter
                           const Numeric      CEin,   // input parameter
                           const String&      model, // model
                           ConstVectorView    f_mono, // frequency vector
                           ConstVectorView    p_abs,  // pressure vector
                           ConstVectorView    t_abs,  // temperature vector
                           ConstVectorView    vmr)    // suspended water droplet density vector
{

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the MPM93 model (J. Liebe and G. A. Hufford and M. G. Cotton,
  // "Propagation modeling of moist air and suspended water/ice
  // particles at frequencies below 1000 GHz",
  // AGARD 52nd Specialists Meeting of the Electromagnetic Wave
  // Propagation Panel, Palma de Mallorca, Spain, 1993, May 17-21)
  const Numeric CC_MPM93 = 1.00000;
  const Numeric CG_MPM93 = 1.00000;
  const Numeric CE_MPM93 = 1.00000;
  // ---------------------------------------------------------------------------------------


  // select the parameter set (!!model dominates values!!):
  Numeric CC, CG, CE;
  if ( model == "MPM93" )
    {
      CC = CC_MPM93;
      CG = CG_MPM93;
      CE = CE_MPM93;
    }
  else if ( model == "user" )
    {
      CC = CCin;
      CG = CGin;
      CE = CEin;
    }
  else
    {
      ostringstream os;
      os << "liquidcloud-MPM93: ERROR! Wrong model values given.\n"
         << "Valid models are: 'MPM93' and 'user'" << '\n';
      throw runtime_error(os.str());
    }
  out3  << "liquidcloud-MPM93: (model=" << model << ") parameter values in use:\n" 
        << " CC = " << CC << "\n"
        << " CG = " << CG << "\n"
        << " CE = " << CE << "\n";
  
  
  const Numeric m = 1.00e3; // specific weight of the droplet,  fixed value:  1.00e3 kg/m³
  const Numeric low_lim_den  =  0.000;   // lower limit of suspended droplet particle density vector [kg/m³]
  const Numeric high_lim_den = 10.00e-3; // lower limit of suspended droplet particle density vector [kg/m³]

  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );
  
  // Loop pressure/temperature:
  for ( Index i=0; i<n_p; ++i )
    {
      // water vapor saturation pressure over liquid water [Pa]
      // Numeric es       = WVSatPressureLiquidWater(t_abs[i]);
      // water vapor partial pressure [Pa]
      // Numeric e        = p_abs[i] * vmr[i];      
      // relative humidity [1]
      // Numeric RH       = e / es;
  
      // Check limits of suspended water droplet density ("vmr") [kg/m³]
      if ( (vmr[i] > low_lim_den) && (vmr[i] < high_lim_den) ) 
        {
          // relative inverse temperature [1]
          Numeric theta    = 300.000 / t_abs[i];
          // relaxation frequencies [GHz]
          Numeric gamma1   = CG * 20.20 - 146.40*(theta-1.000) + 316.00*(theta-1.000)*(theta-1.000);
          // Numeric gamma1  = 20.1 * exp( 7.88 * theta ); // see Liebe et al. IJIMW, 1992, p667, Eq. (2b)
          Numeric gamma2   = 39.80 * gamma1; 
          // static and high-frequency permittivities
          Numeric epsilon0 = CE * 103.30 * (theta-1.000) + 77.66;
          Numeric epsilon1 = 0.0671 * epsilon0;
          Numeric epsilon2 = 3.52;
          
          // Loop frequency:
          for ( Index s=0; s<n_f; ++s )
            {
              // real part of the complex permittivity of water (double-debye model)
              Numeric Reepsilon  = epsilon0 - 
                pow((f_mono[s]*Hz_to_GHz),(Numeric)2.) *
                ( ((epsilon0-epsilon1)/
                   (pow((f_mono[s]*Hz_to_GHz),(Numeric)2.)
                    + pow(gamma1,(Numeric)2.))) + 
                  ((epsilon1-epsilon2)/
                   (pow((f_mono[s]*Hz_to_GHz),(Numeric)2.)
                    + pow(gamma2,(Numeric)2.))) );
              // imaginary part of the complex permittivity of water (double-debye model)
              Numeric Imepsilon  = (f_mono[s]*Hz_to_GHz) *
                ( (gamma1*(epsilon0-epsilon1)/
                   (pow((f_mono[s]*Hz_to_GHz),(Numeric)2.)
                    + pow(gamma1,(Numeric)2.))) + 
                  (gamma2*(epsilon1-epsilon2)/
                   (pow((f_mono[s]*Hz_to_GHz),(Numeric)2.)
                    + pow(gamma2,(Numeric)2.))) );
              // the imaginary part of the complex refractivity of suspended liquid water particle [ppm]
              // In MPM93 w is in g/m³ and m is in g/cm³. Because of the units used in arts,
              // a factor of 1.000e6 must be multiplied with the ratio (w/m):
              // MPM93: (w/m)_MPM93  in   (g/m³)/(g/cm³)
              // arts:  (w/m)_arts   in  (kg/m³)/(kg/m³)
              // =====> (w/m)_MPM93   =   1.0e6 * (w/m)_arts
              // the factor of 1.0e6 is included below in xsec calculation.
              Numeric ImNw = 1.500 / m * 
                ( 3.000 * Imepsilon
                  / ( pow((Reepsilon+(Numeric)2.000),(Numeric)2.)
                      + pow(Imepsilon,(Numeric)2.) ) );
              // liquid water particle absorption cross section [1/m]
              // The vmr of H2O will be multiplied at the stage of absorption 
              // calculation: abs = vmr * xsec.
              // xsec = abs/vmr [1/m] but MPM93 is in [dB/km] --> conversion necessary
              xsec(s,i) += CC * 1.000e6 * dB_km_to_1_m * 0.1820 * (f_mono[s]*Hz_to_GHz) * ImNw;
            }
        } else
          {
            if ( (vmr[i] < low_lim_den) || (vmr[i] > high_lim_den) ) 
              {
                ostringstream os;
                os << "ERROR in MPM93WaterDropletAbs:\n"
                   << " suspended water droplet density (valid range 0.00-10.00e-3 kg/m3):" << vmr[i] << "\n"
                   << " ==> no calculation performed!\n";
                throw runtime_error(os.str());
              }
          }
    }

}
//
// #################################################################################
//
void MPM93IceCrystalAbs( MatrixView        xsec,
                         const Numeric     CCin,   // input parameter
                         const Numeric     CAin,   // input parameter
                         const Numeric     CBin,   // input parameter
                         const String&     model, // model
                         ConstVectorView   f_mono, // frequency vector
                         ConstVectorView   p_abs,  // pressure vector
                         ConstVectorView   t_abs,  // temperature vector
                         ConstVectorView   vmr   ) // suspended ice particle density vector, 
                                                   // valid range: 0-10.0e-3 kg/m³
{

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the MPM93 model (J. Liebe and G. A. Hufford and M. G. Cotton,
  // "Propagation modeling of moist air and suspended water/ice
  // particles at frequencies below 1000 GHz",
  // AGARD 52nd Specialists Meeting of the Electromagnetic Wave
  // Propagation Panel, Palma de Mallorca, Spain, 1993, May 17-21)
  const Numeric CC_MPM93 = 1.00000;
  const Numeric CA_MPM93 = 1.00000;
  const Numeric CB_MPM93 = 1.00000;
  // ---------------------------------------------------------------------------------------


  // select the parameter set (!!model dominates values!!):
  Numeric CC, CA, CB;
  if ( model == "MPM93" )
    {
      CC = CC_MPM93;
      CA = CA_MPM93;
      CB = CB_MPM93;
    }
  else if ( model == "user" )
    {
      CC = CCin;
      CA = CAin;
      CB = CBin;
    }
  else
    {
      ostringstream os;
      os << "icecloud-MPM93: ERROR! Wrong model values given.\n"
         << "Valid models are: 'MPM93' and 'user'" << '\n';
      throw runtime_error(os.str());
    }
  out3  << "icecloud-MPM93: (model=" << model << ") parameter values in use:\n" 
        << " CC = " << CC << "\n"
        << " CA = " << CA << "\n"
        << " CB = " << CB << "\n";
  
  
  const Numeric m = 0.916e3;  // specific weight of ice particles,  fixed value:   0.916e3 kg/m³
  const Numeric low_lim_den  =  0.000;   // lower limit of suspended ice particle density vector [kg/m³]
  const Numeric high_lim_den = 10.00e-3; // lower limit of suspended ice particle density vector [kg/m³]

  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );
  


  // Loop pressure/temperature:
  for ( Index i=0; i<n_p; ++i )
    {
      // water vapor saturation pressure over ice [Pa]
      // Numeric es = WVSatPressureIce(t_abs[i]);
      // water vapor partial pressure [Pa]
      // Numeric e  = p_abs[i] * vmr[i];
      // relative humidity [1]
      // Numeric RH = e / es;
  
      // Check limits of suspended water ice crystal density ("vmr") [kg/m³]
      if ( (vmr[i] > low_lim_den) && (vmr[i] < high_lim_den) ) 
        { 
          // relative inverse temperature [1]
          Numeric theta = 300.000 / t_abs[i];   
          // inverse frequency T-dependency function [Hz]
          Numeric ai = CA * (62.000 * theta - 11.600) * exp(-22.100 * (theta-1.000)) * 1.000e-4;
          // linear frequency T-dependency function [1/Hz]
          Numeric bi = CB * 0.542e-6 * 
                       ( -24.17 + (116.79/theta)
                         + pow((theta/(theta-(Numeric)0.9927)),(Numeric)2.) );
              
          // Loop frequency:
          for ( Index s=0; s<n_f; ++s )
            {
              // real part of the complex permittivity of ice
              Numeric Reepsilon  = 3.15;
              // imaginary part of the complex permittivity of water
              Numeric Imepsilon  = ( ( ai/(f_mono[s]*Hz_to_GHz) ) +
                                     ( bi*(f_mono[s]*Hz_to_GHz) ) );
              // the imaginary part of the complex refractivity of suspended ice particles.
              // In MPM93 w is in g/m³ and m is in g/cm³. Because of the units used in arts,
              // a factor of 1.000e6 must be multiplied with the ratio (w/m):
              // MPM93: (w/m)_MPM93  in   (g/m³)/(g/cm³)
              // arts:  (w/m)_arts   in  (kg/m³)/(kg/m³)
              // =====> (w/m)_MPM93   =   1.0e6 * (w/m)_arts
              // the factor of 1.0e6 is included below in xsec calculation.
              Numeric ImNw = 1.500 / m * 
                    ( 3.000 * Imepsilon
                      / ( pow((Reepsilon+(Numeric)2.000),(Numeric)2.)
                          + pow(Imepsilon,(Numeric)2.) ) );
              // ice particle absorption cross section [1/m]
              // The vmr of H2O will be multiplied at the stage of absorption 
              // calculation: abs = vmr * xsec.
              // xsec = abs/vmr [1/m] but MPM93 is in [dB/km] --> conversion necessary
              xsec(s,i) += CC * 1.000e6 * dB_km_to_1_m * 0.1820 * (f_mono[s]*Hz_to_GHz) * ImNw;
            }
        } else
          {
            if ( (vmr[i] < low_lim_den) || (vmr[i] > high_lim_den) ) 
              {
                ostringstream os;
                os << "ERROR in MPM93IceCrystalAbs:\n"
                   << " suspended ice particle density (valid range: 0-10.0e-3 kg/m3):" << vmr[i] << "\n"
                   << " ==> no calculation performed!\n";
                throw runtime_error(os.str());
              }
          }
    }
  return;
}
//
// #################################################################################
//
void MPM93RainExt( MatrixView         xsec,
                   const Numeric      CEin,   // input parameter
                   const Numeric      CAin,   // input parameter
                   const Numeric      CBin,   // input parameter
                   const String&      model, // model
                   ConstVectorView    f_mono, // frequency vector
                   ConstVectorView    p_abs,  // pressure vector
                   ConstVectorView    t_abs,  // temperature vector
                   ConstVectorView    vmr)    // rain rate profile [mm/h]
{

  // --------- STANDARD MODEL PARAMETERS ---------------------------------------------------
  // standard values for the MPM93 model based on Olsen, R.L.,
  // D.V. Rogers, and D. B. Hodge, "The aR^b relation in the
  // calculation of rain attenuation", IEEE Trans. Antennas Propagat.,
  // vol. AP-26, pp. 318-329, 1978,
  const Numeric CE_MPM93 = 1.00000;
  const Numeric CA_MPM93 = 1.00000;
  const Numeric CB_MPM93 = 1.00000;
  // ---------------------------------------------------------------------------------------


  // select the parameter set (!!model dominates values!!):
  Numeric CE, CA, CB;
  if ( model == "MPM93" )
    {
      CE = CE_MPM93;
      CA = CA_MPM93;
      CB = CB_MPM93;
    }
  else if ( model == "user" )
    {
      CE = CEin;
      CA = CAin;
      CB = CBin;
    }
  else
    {
      ostringstream os;
      os << "rain-MPM93: ERROR! Wrong model values given.\n"
         << "Valid models are: 'MPM93' and 'user'" << '\n';
      throw runtime_error(os.str());
    }
  out3  << "rain-MPM93: (model=" << model << ") parameter values in use:\n" 
        << " CE = " << CE << "\n"
        << " CA = " << CA << "\n"
        << " CB = " << CB << "\n";
  
  
  const Numeric low_lim_rr  =  0.000;   // lower limit of allowed rain rate  [mm/h]
  const Numeric high_lim_rr = 150.000;  // upper limit of allowed rain rate  [mm/h]

  const Index n_p = p_abs.nelem();      // Number of pressure levels
  const Index n_f = f_mono.nelem();     // Number of frequencies

  // Check that dimensions of p_abs, t_abs, and vmr agree:
  assert ( n_p==t_abs.nelem() );
  assert ( n_p==vmr.nelem()   );

  // Check that dimensions of xsec are consistent with n_f
  // and n_p. It should be [n_f,n_p]:
  assert ( n_f==xsec.nrows() );
  assert ( n_p==xsec.ncols() );
  
  // Loop pressure/temperature:
  for ( Index i=0; i<n_p; ++i )
    {
      // Extinction by rain is parameterized as:
      //  ext_rain = a_rain * rr ^ b_rain
      // a_rain and b_rain each depend on frequency by  power laws:
      //  a_rain = Ga * freq ^ Ea
      //  b_rain = Gb * freq ^ Eb
      Numeric Ga = 0.;
      Numeric Ea = 0.;
      Numeric Gb = 0.;
      Numeric Eb = 0.;
      // FIXME Numeric a_rain;
      // FIXME Numeric b_rain;
      // FIXME Numeric ext_rain;

      // Check limits of rain rate ("vmr") [mm/h]
      if ( (vmr[i] >= low_lim_rr) && (vmr[i] < high_lim_rr) ) 
        {
          // Loop frequency:
          for ( Index s=0; s<n_f; ++s )
            {
              // for rain rate < 25 mm/h, take parameters from Olsen et al.'s
              // own power law fit to their Laws-Parsons-Low data;
              // for rain rate > 25 mm/h, take C. Melsheimer's power law fit
              // to Olsen et al.'s Laws-Parson-High data
              if ( vmr[i] <= 25 ) 
                {             
                  // power law coeff. Ga and exponent Ea for a, piecewise:
                  if ( f_mono[s] <= 2.9e9 ) 
                    {
                      Ga = 6.39e-5;
                      Ea = 2.03;
                    }
                  else if ( f_mono[s] <= 54.0e9 )
                    {
                      Ga = 4.21e-5;
                      Ea = 2.42;
                    }
                  else if ( f_mono[s] <= 180e9 )
                    {
                      Ga = 4.09e-2;
                      Ea = 0.699;
                    }
                  else if ( f_mono[s] <= 1000e9 )
                    {
                      Ga = 3.38;
                      Ea = -0.151;
                    }
                  else 
                    {
                      ostringstream os;
                      os << "ERROR in MPM93RainExt:\n"
                         << " frequency (valid range 0-1000 GHz):" << f_mono[s]*Hz_to_GHz << "\n"
                         << " ==> no calculation performed!\n";
                      throw runtime_error(os.str());
                    }
                  // power law coeff. Gb and exponent Eb for b, piecewise:
                  if ( f_mono[s] <= 8.5e9 ) 
                    {
                      Gb = 0.851;
                      Eb = 0.158;
                    }
                  else if ( f_mono[s] <= 25.0e9 )
                    {
                      Gb = 1.41;           
                      Eb = -0.0779;
                    }
                  else if ( f_mono[s] <= 164.0e9 )
                    {
                      Gb = 2.63;          
                      Eb = -0.272;
                    }
                  else if ( f_mono[s] <= 1000e9 )
                    {
                      Gb = 0.616;
                      Eb = 0.0126;
                    }
                  else 
                    {
                      ostringstream os;
                      os << "ERROR in MPM93RainExt:\n"
                         << " frequency (valid range 0-1000 GHz):" << f_mono[s]*Hz_to_GHz << "\n"
                         << " ==> no calculation performed!\n";
                      throw runtime_error(os.str());
                    }
                  
                }
              else if (vmr[i] > 25)
                {
                  // power law coeff. Ga and exponent Ea for a, piecewise:
                  if ( f_mono[s] <= 4.9e9 ) 
                    {
                      Ga = 5.30e-5;
                      Ea = 1.87;
                    }
                  else if ( f_mono[s] <= 10.7e9 )
                    {
                      Ga = 5.03e-6;
                      Ea = 3.35;
                    }
                  else if ( f_mono[s] <= 40.1e9 )
                    {
                      Ga = 2.53e-5;
                      Ea = 2.67;
                    }
                  else if ( f_mono[s] <= 59.1e9 )
                    {
                      Ga = 3.58e-3;
                      Ea = 1.33;
                    }
                  else if ( f_mono[s] <= 100e9 )
                    {
                      Ga = 0.143;
                      Ea = 0.422;
                    }
                  else 
                    {
                      ostringstream os;
                      os << "ERROR in MPM93RainExt:\n"
                         << " frequency (valid range for rain rate > 25mm/h: 0-100 GHz):" << f_mono[s]*Hz_to_GHz << "\n"
                         << " ==> no calculation performed!\n";
                      throw runtime_error(os.str());
                    }
                  // power law coeff. Gb and exponent Eb for b, piecewise:
                  if ( f_mono[s] <= 6.2e9 ) 
                    {
                      Gb = 0.911;
                      Eb = 0.190;
                    }
                  else if ( f_mono[s] <= 23.8e9 )
                    {
                      Gb = 1.71;           
                      Eb = -0.156;
                    }
                  else if ( f_mono[s] <= 48.4e9 )
                    {
                      Gb = 3.08;          
                      Eb = -0.342;
                    }
                  else if ( f_mono[s] <= 68.2e9 )
                    {
                      Gb = 1.28;
                      Eb = -0.116;
                    }
                  else if ( f_mono[s] <= 100e9 )
                    {
                      Gb =  0.932;
                      Eb =  -0.0408;
                    }
                  else 
                    {
                      ostringstream os;
                      os << "ERROR in MPM93RainExt:\n"
                         << " frequency (valid range for rain rate > 25mm/h: 0-100 GHz):" << f_mono[s]*Hz_to_GHz << "\n"
                         << " ==> no calculation performed!\n";
                      throw runtime_error(os.str());
                    }
                }
              //Factor a_rain
              Numeric a_rain = Ga * pow((f_mono[s]*Hz_to_GHz),Ea);
              //Factor b_rain
              Numeric b_rain = Gb * pow((f_mono[s]*Hz_to_GHz),Eb);
              // Extinction coefficient [dB/km], with scaling
              // parameters CA and CB
              Numeric ext_rain = CA * a_rain * pow(vmr[i],(CB*b_rain));
              // rain extinction cross section [1/m]
              // The vmr will be multiplied at the stage of extinction
              // calculation: ext = vmr * xsec.
              // xsec = ext/vmr [1/m] but MPM93 is in [dB/km] --> conversion necessary
              xsec(s,i) += CE * dB_km_to_1_m * ext_rain / vmr[i];
            }
        } else
          {
            if ( (vmr[i] < low_lim_rr) || (vmr[i] > high_lim_rr) ) 
              {
                ostringstream os;
                os << "ERROR in MPM93RainExt:\n"
                   << " rain rate (valid range 0.00-150.00 mm/h):" << vmr[i] << "\n"
                   << " ==> no calculation performed!\n";
                throw runtime_error(os.str());
              }
          }
    }
  
}
//
// #################################################################################
// ################################# HELP FUNCTIONS ################################
// #################################################################################
//
Numeric MPMLineShapeFunction( const Numeric gamma, 
                              const Numeric fl, 
                              const Numeric f)
{
  /*
    this routine calculates the line shape function of Van Vleck and Weisskopf
    with the factor (f/f_o)¹. for the MPM pseudo continuum line.

    creation  TKS, 4.11.00 

    input:   gamma   [Hz]    line width of line L
             fl      [Hz]    central frequency of line L
             f       [Hz]    frequency position of calculation
             
    output:  value   [1/Hz]  line shape function value at f for the line parameters
                              of line L 
              
   */

  double f_minus, f_plus ;           /* internal variables */
  double value;                      /* return value       */

  // line at fl
  f_minus = 1.000 / ((f-fl)*(f-fl) + gamma*gamma);

  // mirror line at -fl
  f_plus  = 1.000 / ((f+fl)*(f+fl) + gamma*gamma);

  // VVW line shape function value
  value = fabs(f/fl) * gamma * (f_minus + f_plus);
  
  return value;
}
//
// #################################################################################
//
Numeric MPMLineShapeO2Function( const Numeric gamma, 
                                const Numeric fl, 
                                const Numeric f,
                                const Numeric delta)
{
  /*
    this routine calculates the line shape function of Van Vleck and Weisskopf
    for O2 with line mixing.

    creation  TKS, 14.07.01 

    input:   gamma   [GHz]    line width of line L
             fl      [GHz]    central frequency of line L
             f       [GHz]    frequency position of calculation
             delta   [1]     line mixing parameter
             
    output:  value   [1]     line shape function value at f for the line parameters
                             of line L 
              
   */

  double f_minus, f_plus ;           /* internal variables */
  double value;                      /* return value       */

  // line at fl
  f_minus = (gamma - delta * (fl-f)) / ((fl-f)*(fl-f) + gamma*gamma);

  // mirror line at -fl
  f_plus  = (gamma - delta * (fl+f)) / ((fl+f)*(fl+f) + gamma*gamma);

  // VVW line shape function value
  value = f * (f_minus + f_plus);
  
  return value;
}
//
// #################################################################################
//
Numeric WVSatPressureLiquidWater(const Numeric t)
{

  // check of temperature range
  if (t < 0.000)
    {
      ostringstream os;
      os << "In WVSatPressureLiquidWater:\n"
         << "temperature negative: T=" << t <<"K \n";
      throw runtime_error(os.str());
    }

  //  COMPUTES SATURATION H2O VAPOR PRESSURE (OVER LIQUID)
  //  USING LIEBE'S APPROXIMATION (CORRECTED)
  //  input  : T in Kelvin
  //  output : es in Pa
  //  PWR 4/8/92
  /*
  Numeric TH       = 300.0 / t;
  Numeric es_PWR98 = 100.00 * 35.3 * exp(22.64*(1.-TH)) * pow(TH,5.0);
  */

  // MPM93 calculation
  Numeric theta    = 373.16 / t;
  Numeric exponent = ( -7.90298 * (theta-1.000) +
                        5.02808 * log10(theta) -
                        1.3816e-7 * ( pow( (Numeric)10.00,
                                           ((Numeric)11.344*
                                            ((Numeric)1.00-((Numeric)1.00
                                                             /theta))) )
                                      - (Numeric)1.000 ) +
                        8.1328e-3 * ( pow( (Numeric)10.00,
                                           ((Numeric)-3.49149
                                            *(theta-(Numeric)1.00)))
                                      - 1.000) +
                        log10(1013.246) );
  Numeric es_MPM93 = 100.000 * pow((Numeric)10.00,exponent);

  return es_MPM93; // [Pa]
}
//
// #################################################################################
//
Numeric WVSatPressureIce(const Numeric t)
{

  // check of temperature range
  if (t < 0.000)
    {
      ostringstream os;
      os << "In WVSatPressureIce:\n"
         << "temperature negative: T=" << t <<"K \n";
      throw runtime_error(os.str());
    }

  // MPM93 calculation
  Numeric theta    = 273.16 / t;
  Numeric exponent = (-9.09718  * (theta-1.000) -
                       3.56654  * log10(theta)  +
                       0.876793 * (1.000-(1.000/theta)) +
                       log10(6.1071) );

  Numeric es_MPM93 = 100.000 * pow((Numeric)10.00,exponent);

  return es_MPM93;
}
//
// #################################################################################
// #################### CONTROL OF ADDITIONAL ABSORPTION MODEL #####################
// #################################################################################
//
//
void xsec_continuum_tag( MatrixView                 xsec,
                         const String&              name,
                         ConstVectorView            parameters,
                         const String&              model,
                         ConstVectorView            f_mono,
                         ConstVectorView            p_abs,
                         ConstVectorView            t_abs,
                         ConstVectorView            n2_abs,
                         ConstVectorView            h2o_abs,
                         ConstVectorView            vmr )
{
  //
  /* In the following all the possible tags are listed here and 
   after a first consistency check about the input parameters the 
   appropriate internal function is called,

  !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! 
  ATTENTION PLEASE UPDATE THIS COMMENT IF ANY CHANGES ARE MADE CONCERNING 
  THE ASSOCIATED MODELS TO EACH TAG
  !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!

  ----------------------------------------------------------------------------------------------------
                    TAG                      VALID MODELS  
  ----------------------------------------------------------------------------------------------------
  *CONTAGMODINFO*   H2O-SelfContStandardType: Rosenkranz, user
  *CONTAGMODINFO*   H2O-ForeignContStandardType: Rosenkranz, user
  *CONTAGMODINFO*   H2O-ForeignContMaTippingType: MaTipping, user
  *CONTAGMODINFO*   H2O-MPM87:               MPM87, MPM87Lines, MPM87Continuum, user
  *CONTAGMODINFO*   H2O-MPM89:               MPM89, MPM89Lines, MPM89Continuum, user
  *CONTAGMODINFO*   H2O-MPM93:               MPM93, MPM93Lines, MPM93Continuum, user
  *CONTAGMODINFO*   H2O-PWR98:               Rosenkranz, RosenkranzLines, RosenkranzContinuum, user
  *CONTAGMODINFO*   H2O-CP98:                CruzPol, CruzPolLine, CruzPolContinuum, user
  *CONTAGMODINFO*   H2O-CKD24:               CKD24, user
  *CONTAGMODINFO*   O2-MPM85:                MPM85, MPM85Lines, MPM85Continuum, MPM85NoCoupling, MPM85NoCutoff, user
  *CONTAGMODINFO*   O2-MPM87:                MPM87, MPM87Lines, MPM87Continuum, MPM87NoCoupling, MPM87NoCutoff, user
  *CONTAGMODINFO*   O2-MPM89:                MPM89, MPM89Lines, MPM89Continuum, MPM89NoCoupling, MPM89NoCutoff, user
  *CONTAGMODINFO*   O2-MPM92:                MPM92, MPM92Lines, MPM92Continuum, MPM92NoCoupling, MPM92NoCutoff, user
  *CONTAGMODINFO*   O2-MPM93:                MPM93, MPM93Lines, MPM93Continuum, MPM93NoCoupling, MPM92NoCutoff, user
  *CONTAGMODINFO*   O2-PWR93:                Rosenkranz, RosenkranzLines, RosenkranzContinuum, user
  *CONTAGMODINFO*   O2-PWR88:                Rosenkranz, RosenkranzLines, RosenkranzContinuum, user
  *CONTAGMODINFO*   O2-SelfContMPM93:        MPM93, user
  *CONTAGMODINFO*   O2-SelfContPWR93:        Rosenkranz, user
  *CONTAGMODINFO*   O2-GenerealCont:         Rosenkranz, MPM93, user
  *CONTAGMODINFO*   N2-BFCIA86:              BF86, user
  *CONTAGMODINFO*   N2-SelfContMPM93:        MPM93, user, MPM93Scale
  *CONTAGMODINFO*   N2-SelfContPWR93:        Rosenkranz, user
  *CONTAGMODINFO*   N2-SelfContStandardType: Rosenkranz, user
  *CONTAGMODINFO*   CO2-SelfContPWR93:       Rosenkranz, user
  *CONTAGMODINFO*   CO2-ForeignContPWR93:    Rosenkranz, user
  *CONTAGMODINFO*   liquidcloud-MPM93:       MPM93, user
  *CONTAGMODINFO*   icecloud-MPM93:          MPM93, user
  *CONTAGMODINFO*   rain-MPM93:              MPM93, user
  ----------------------------------------------------------------------------------------------------
  */
  // ============= H2O continuum ========================================================
  if ( "H2O-SelfContStandardType"==name )
    {
      // 
      //  specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT
      //     parameters[0] : continuum coefficient (C_s)  [1/m / (Hz²*Pa²)]
      //     parameters[1] : temperature exponent  (x_s)  [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     vmr           : [1]
      //
      const int Nparam = 2;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          Standard_H2O_self_continuum( xsec,
                                       parameters[0],
                                       parameters[1],
                                       model,
                                       f_mono,
                                       p_abs,
                                       t_abs,
                                       vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          Standard_H2O_self_continuum( xsec,
                                       0.00,
                                       0.00,
                                       model,
                                       f_mono,
                                       p_abs,
                                       t_abs,
                                       vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "H2O-ForeignContStandardType"==name )
    {
      //      
      // specific continuum parameters units:
      //  a) output 
      //     xsec          : [1/m],
      //  b) input
      //     parameters[0] : [1/m / (Hz²*Pa²)]
      //     parameters[1] : [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     vmr           : [1]
      //
      const int Nparam = 2;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          Standard_H2O_foreign_continuum( xsec,
                                          parameters[0],
                                          parameters[1],
                                          model,
                                          f_mono,
                                          p_abs,
                                          t_abs,
                                          vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          Standard_H2O_foreign_continuum( xsec,
                                          0.00,
                                          0.00,
                                          model,
                                          f_mono,
                                          p_abs,
                                          t_abs,
                                          vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "H2O-ForeignContMaTippingType"==name )
    {
      //      
      // specific continuum parameters units:
      //  a) output 
      //     xsec          : [1/m],
      //  b) input
      //     parameters[0] : [1/m / (Hz²*Pa²)]
      //     parameters[1] : [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     vmr           : [1]
      //
      const int Nparam = 2;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          MaTipping_H2O_foreign_continuum( xsec,
                                           parameters[0],
                                           parameters[1],
                                           model,
                                           f_mono,
                                           p_abs,
                                           t_abs,
                                          vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          MaTipping_H2O_foreign_continuum( xsec,
                                           0.00,
                                           0.00,
                                           model,
                                           f_mono,
                                           p_abs,
                                           t_abs,
                                           vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "H2O-ContMPM93"==name )
    {
      // self and foreign continuum term are simultaneously calculated
      // since the parameterization can not be divided up in these two 
      // terms because they are not additive terms.
      //
      // specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT
      //     parameters[0] : pseudo continuum line frequency                      [Hz]
      //     parameters[1] : pseudo continuum line strength parameter             [Hz/Pa]
      //     parameters[2] : pseudo continuum line strength temperature parameter [1]
      //     parameters[3] : pseudo continuum line broadening parameter           [Hz/Pa]
      //     parameters[4] : pseudo continuum line broadening parameter           [1]
      //     parameters[5] : pseudo continuum line broadening parameter           [1]
      //     parameters[6] : pseudo continuum line broadening parameter           [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     vmr           : [1]
      //
      const int Nparam = 7;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          MPM93_H2O_continuum( xsec,
                               parameters[0],
                               parameters[1],
                               parameters[2],
                               parameters[3],
                               parameters[4],
                               parameters[5],
                               parameters[6],
                               model,
                               f_mono,
                               p_abs,
                               t_abs,
                               vmr       );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          MPM93_H2O_continuum( xsec,
                               0.00,
                               0.00,
                               0.00,
                               0.00,
                               0.00,
                               0.00,
                               0.00,
                               model,
                               f_mono,
                               p_abs,
                               t_abs,
                               vmr       );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters. " << "\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "H2O-ForeignContATM01"==name )
    {
      // Foreign wet continuum term.
      //
      // Pardo et al., IEEE, Trans. Ant. Prop., 
      // Vol 49, No 12, pp. 1683-1694, 2001.
      //
      // specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT
      //     parameters[0] : pseudo continuum line frequency                      [Hz]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     vmr           : [1]
      //
      const int Nparam = 1;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          Pardo_ATM_H2O_ForeignContinuum( xsec,
                                          parameters[0],
                                          model,
                                          f_mono,
                                          p_abs,
                                          t_abs,
                                          vmr    );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          Pardo_ATM_H2O_ForeignContinuum( xsec,
                                          0.000,
                                          model,
                                          f_mono,
                                          p_abs,
                                          t_abs,
                                          vmr    );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters. " << "\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "H2O-SelfContCKD222"==name )
    {
      // OUTPUT:
      //   xsec           cross section (absorption/volume mixing ratio) of 
      //                  H2O self continuum according to CKD2.2.2    [1/m]
      // INPUT:
      //   parameters[0]  strength scaling factor              [1]
      //   model          allows user defined input parameter set 
      //                  (Cin) or choice of 
      //                  pre-defined parameters of specific models (see note below).
      //   f_mono         predefined frequency grid            [Hz]
      //   p_abs          predefined pressure grid             [Pa]
      //   t_abs          predefined temperature grid          [K] 
      //   vmr            H2O volume mixing ratio profile      [1]
      //   n2_abs         N2 volume mixing ratio profile       [1]
      //
      // WWW resource: ftp.aer.com/aer_contnm_ckd
      const int Nparam = 1;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          CKD_222_self_h2o( xsec,
                            parameters[0],
                            model,
                            f_mono,
                            p_abs,
                            t_abs,
                            vmr,
                            n2_abs );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          CKD_222_self_h2o( xsec,
                            0.000,
                            model,
                            f_mono,
                            p_abs,
                            t_abs,
                            vmr,
                            n2_abs );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
       {
          ostringstream os;
          os << "ERROR: continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
       }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "H2O-ForeignContCKD222"==name )
    {
      // OUTPUT:
      //   xsec           cross section (absorption/volume mixing ratio) of 
      //                  H2O foreign continuum according to CKD2.2.2    [1/m]
      // INPUT:
      //   parameters[0]  strength scaling factor              [1]
      //   model          allows user defined input parameter set 
      //                  (Cin) or choice of 
      //                  pre-defined parameters of specific models (see note below).
      //   f_mono         predefined frequency grid            [Hz]
      //   p_abs          predefined pressure grid             [Pa]
      //   t_abs          predefined temperature grid          [K] 
      //   vmr            H2O volume mixing ratio profile      [1]
      //   n2_abs         N2 volume mixing ratio profile       [1]
      //
      // WWW resource: ftp.aer.com/aer_contnm_ckd
      const int Nparam = 1;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          CKD_222_foreign_h2o( xsec,
                               parameters[0],
                               model,
                               f_mono,
                               p_abs,
                               t_abs,
                               vmr,
                               n2_abs );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          CKD_222_foreign_h2o( xsec,
                               0.000,
                               model,
                               f_mono,
                               p_abs,
                               t_abs,
                               vmr,
                               n2_abs );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
       {
          ostringstream os;
          os << "ERROR: continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
       }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "H2O-SelfContCKD242"==name )
    {
      // OUTPUT:
      //   xsec           cross section (absorption/volume mixing ratio) of 
      //                  H2O self continuum according to CKD2.4.2    [1/m]
      // INPUT:
      //   parameters[0]  strength scaling factor              [1]
      //   model          allows user defined input parameter set 
      //                  (Cin) or choice of 
      //                  pre-defined parameters of specific models (see note below).
      //   f_mono         predefined frequency grid            [Hz]
      //   p_abs          predefined pressure grid             [Pa]
      //   t_abs          predefined temperature grid          [K] 
      //   vmr            H2O volume mixing ratio profile      [1]
      //   n2_abs         N2 volume mixing ratio profile       [1]
      //
      // WWW resource: ftp.aer.com/aer_contnm_ckd
      const int Nparam = 1;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          CKD_242_self_h2o( xsec,
                            parameters[0],
                            model,
                            f_mono,
                            p_abs,
                            t_abs,
                            vmr,
                            n2_abs );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          CKD_242_self_h2o( xsec,
                            0.000,
                            model,
                            f_mono,
                            p_abs,
                            t_abs,
                            vmr,
                            n2_abs );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
       {
          ostringstream os;
          os << "ERROR: continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
       }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "H2O-ForeignContCKD242"==name )
    {
      // OUTPUT:
      //   xsec           cross section (absorption/volume mixing ratio) of 
      //                  H2O foreign continuum according to CKD2.4.2    [1/m]
      // INPUT:
      //   parameters[0]  strength scaling factor              [1]
      //   model          allows user defined input parameter set 
      //                  (Cin) or choice of 
      //                  pre-defined parameters of specific models (see note below).
      //   f_mono         predefined frequency grid            [Hz]
      //   p_abs          predefined pressure grid             [Pa]
      //   t_abs          predefined temperature grid          [K] 
      //   vmr            H2O volume mixing ratio profile      [1]
      //   n2_abs         N2 volume mixing ratio profile       [1]
      //
      // WWW resource: ftp.aer.com/aer_contnm_ckd
      const int Nparam = 1;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          CKD_242_foreign_h2o( xsec,
                               parameters[0],
                               model,
                               f_mono,
                               p_abs,
                               t_abs,
                               vmr,
                               n2_abs );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          CKD_242_foreign_h2o( xsec,
                               0.000,
                               model,
                               f_mono,
                               p_abs,
                               t_abs,
                               vmr,
                               n2_abs );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
       }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "H2O-SelfContCKDMT100"==name )
    {
      // OUTPUT:
      //   xsec           cross section (absorption/volume mixing ratio) of 
      //                  H2O self continuum according to CKD MT 1.00    [1/m]
      // INPUT:
      //   parameters[0]  strength scaling factor              [1]
      //   model          allows user defined input parameter set 
      //                  (Cin) or choice of 
      //                  pre-defined parameters of specific models (see note below).
      //   f_mono         predefined frequency grid            [Hz]
      //   p_abs          predefined pressure grid             [Pa]
      //   t_abs          predefined temperature grid          [K] 
      //   vmr            H2O volume mixing ratio profile      [1]
      //   n2_abs         N2 volume mixing ratio profile       [1]
      //
      // WWW resource: ftp.aer.com/aer_contnm_ckd
      const int Nparam = 1;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          CKD_mt_100_self_h2o( xsec,
                               parameters[0],
                               model,
                               f_mono,
                               p_abs,
                               t_abs,
                               vmr,
                               n2_abs );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          CKD_mt_100_self_h2o( xsec,
                               0.000,
                               model,
                               f_mono,
                               p_abs,
                               t_abs,
                               vmr,
                               n2_abs );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
       {
          ostringstream os;
          os << "ERROR: continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
       }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "H2O-ForeignContCKDMT100"==name )
    {
      // OUTPUT:
      //   xsec           cross section (absorption/volume mixing ratio) of 
      //                  H2O foreign continuum according to CKD MT 1.00    [1/m]
      // INPUT:
      //   parameters[0]  strength scaling factor              [1]
      //   model          allows user defined input parameter set 
      //                  (Cin) or choice of 
      //                  pre-defined parameters of specific models (see note below).
      //   f_mono         predefined frequency grid            [Hz]
      //   p_abs          predefined pressure grid             [Pa]
      //   t_abs          predefined temperature grid          [K] 
      //   vmr            H2O volume mixing ratio profile      [1]
      //   n2_abs         N2 volume mixing ratio profile       [1]
      //
      // WWW resource: ftp.aer.com/aer_contnm_ckd
      const int Nparam = 1;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          CKD_mt_100_foreign_h2o( xsec,
                                  parameters[0],
                                  model,
                                  f_mono,
                                  p_abs,
                                  t_abs,
                                  vmr,
                                  n2_abs );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          CKD_mt_100_foreign_h2o( xsec,
                                  0.000,
                                  model,
                                  f_mono,
                                  p_abs,
                                  t_abs,
                                  vmr,
                                  n2_abs );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
       }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "H2O-SelfContCKD24"==name )
    {
      // OUTPUT:
      //   xsec           cross section (absorption/volume mixing ratio) of 
      //                  H2O continuum according to CKD2.4    [1/m]
      // INPUT:
      //   parameters[0]  strength scaling factor              [1]
      //   model          allows user defined input parameter set 
      //                  (Cin) or choice of 
      //                  pre-defined parameters of specific models (see note below).
      //   f_mono         predefined frequency grid            [Hz]
      //   p_abs          predefined pressure grid             [Pa]
      //   t_abs          predefined temperature grid          [K] 
      //   vmr            H2O volume mixing ratio profile      [1]
      //   n2_abs         N2 volume mixing ratio profile       [1]
      //
      // WWW resource: ftp.aer.com/aer_contnm_ckd
      const int Nparam = 1;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          CKD24_H20( xsec,
                     0,
                     parameters[0],
                     model,
                     f_mono,
                     p_abs,
                     t_abs,
                     vmr,
                     n2_abs );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          CKD24_H20( xsec,
                     0,
                     0.000,
                     model,
                     f_mono,
                     p_abs,
                     t_abs,
                     vmr,
                     n2_abs );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
       {
          ostringstream os;
          os << "ERROR: continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
       }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "H2O-ForeignContCKD24"==name ) 
    {
      // OUTPUT:
      //   xsec             cross section (absorption/volume mixing ratio) of 
      //                    H2O continuum according to CKD2.4    [1/m]
      // INPUT:
      //   Cin            strength scaling factor              [1]
      //   model          allows user defined input parameter set 
      //                  (Cin) or choice of 
      //                  pre-defined parameters of specific models (see note below).
      //   f_mono         predefined frequency grid            [Hz]
      //   p_abs          predefined pressure grid             [Pa]
      //   t_abs          predefined temperature grid          [K] 
      //   vmr            H2O volume mixing ratio profile      [1]
      //   n2_abs         N2 volume mixing ratio profile       [1]
      //
      // WWW resource: ftp.aer.com/aer_contnm_ckd
      const int Nparam = 1;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          CKD24_H20( xsec,
                     1,
                     parameters[0],
                     model,
                     f_mono,
                     p_abs,
                     t_abs,
                     vmr,
                     n2_abs );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          CKD24_H20( xsec,
                     1,
                     0,
                     model,
                     f_mono,
                     p_abs,
                     t_abs,
                     vmr,
                     n2_abs );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
        }
    }
  // ============= H2O full models ======================================================
  else if ( "H2O-CP98"==name )
    {
      //
      // specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT
      //     parameters[0] : continuum scale factor       (CC) [1]
      //     parameters[1] : line strength scale factor   (CL) [1]
      //     parameters[2] : line broadening scale factor (CW) [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     vmr           : [1]
      //
      const int Nparam = 3;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Full model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          CP98H2OAbsModel( xsec,
                           parameters[0],
                           parameters[1],
                           parameters[2],
                           model,
                           f_mono,
                           p_abs,
                           t_abs,
                           vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Full model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Full model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          CP98H2OAbsModel( xsec,
                           0.00,
                           0.00,
                           0.00,
                           model,
                           f_mono,
                           p_abs,
                           t_abs,
                           vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Full model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "H2O-MPM87"==name )
    {
      //
      // specific continuum parameters and units:
      //  a) output 
      //     xsec          : [1/m],
      //  b) input
      //     parameters[0] : continuum scale factor (CC)       [1]
      //     parameters[1] : line strength scale factor   (CL) [1]
      //     parameters[2] : line broadening scale factor (CW) [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     vmr           : [1]
      //
      const int Nparam = 3;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Full model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          MPM87H2OAbsModel( xsec,
                            parameters[0],
                            parameters[1],
                            parameters[2],
                            model,
                            f_mono,
                            p_abs,
                            t_abs,
                            vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Full model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Full model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          MPM87H2OAbsModel( xsec,
                            0.00,
                            0.00,
                            0.00,
                            model,
                            f_mono,
                            p_abs,
                            t_abs,
                            vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Full model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "H2O-MPM89"==name )
    {
      //
      // specific continuum parameters and units:
      //  a) output 
      //     xsec          : [1/m],
      //  b) input
      //     parameters[0] : continuum scale factor       (CC) [1]
      //     parameters[1] : line strength scale factor   (CL) [1]
      //     parameters[2] : line broadening scale factor (CW  [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     vmr           : [1]
      //
      const int Nparam = 3;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Full model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          MPM89H2OAbsModel( xsec,
                        parameters[0],
                        parameters[1],
                        parameters[2],
                        model,
                        f_mono,
                        p_abs,
                        t_abs,
                        vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Full model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Full model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          MPM89H2OAbsModel( xsec,
                            0.00,
                            0.00,
                            0.00,
                            model,
                            f_mono,
                            p_abs,
                            t_abs,
                            vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Full model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "H2O-MPM93"==name )
    {
      //
      // specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT
      //     parameters[0] : continuum scale factor       (CC) [1]
      //     parameters[1] : line strength scale factor   (CL) [1]
      //     parameters[2] : line broadening scale factor (CW) [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     vmr           : [1]
      //
      const int Nparam = 3;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Full model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          MPM93H2OAbsModel( xsec,
                            parameters[0],
                            parameters[1],
                            parameters[2],
                            model,
                            f_mono,
                            p_abs,
                            t_abs,
                            vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Full model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Full model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          MPM93H2OAbsModel( xsec,
                            0.00,
                            0.00,
                            0.00,
                            model,
                            f_mono,
                            p_abs,
                            t_abs,
                            vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Full model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "H2O-PWR98"==name )
    {      
      // specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT
      //     parameters[0] : continuum scale factor       (CC) [1]
      //     parameters[1] : line strength scale factor   (CL) [1]
      //     parameters[2] : line broadening scale factor (CW) [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     vmr           : [1]
      //
      const int Nparam = 3;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Full model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          PWR98H2OAbsModel( xsec,
                            parameters[0],
                            parameters[1],
                            parameters[2],
                            model,
                            f_mono,
                            p_abs,
                            t_abs,
                            vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Full model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Full model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          PWR98H2OAbsModel( xsec,
                            0.00,
                            0.00,
                            0.00,
                            model,
                            f_mono,
                            p_abs,
                            t_abs,
                            vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Full model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ============= O2 continuum =========================================================
  else if ( "O2-CIAfunCKDMT100"==name )
    {
      // Model reference:
      // F. Thibault, V. Menoux, R. Le Doucen, L. Rosenman, 
      // J.-M. Hartmann, Ch. Boulet, 
      // "Infrared collision-induced absorption by O2 near 6.4 microns for
      // atmospheric applications: measurements and emprirical modeling", 
      // Appl. Optics, 35, 5911-5917, (1996).
      //
      //  specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT
      //     parameters[0] : continuum scaling
      //     model         : model option ("CKD" or "user")
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     h2o_abs       : [1]
      //     vmr           : [1]
      //
      const int Nparam = 1;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          CKD_mt_CIAfun_o2( xsec,
                            parameters[0],
                            model, 
                            f_mono,
                            p_abs,
                            t_abs,
                            vmr );
        }  
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          CKD_mt_CIAfun_o2( xsec,
                            0.00e0,
                            model, 
                            f_mono,
                            p_abs,
                            t_abs,
                            vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "O2-v0v0CKDMT100"==name )
    {
      // Model reference:
      //   B. Mate, C. Lugez, G.T. Fraser, W.J. Lafferty,
      //   "Absolute Intensities for the O2 1.27 micron
      //   continuum absorption",  
      //   J. Geophys. Res., 104, 30,585-30,590, 1999. 
      //
      //  specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT
      //     parameters[0] : continuum scaling
      //     model         : model option ("CKD" or "user")
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     vmr           : [1]
      //     n2_abs        : [1]
      //     h2o_abs       : [1]
      //
      const int Nparam = 1;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          CKD_mt_v0v0_o2( xsec,
                          parameters[0],
                          model, 
                          f_mono,
                          p_abs,
                          t_abs,
                          vmr,
                          n2_abs );
        }  
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          CKD_mt_v0v0_o2( xsec,
                          0.0e0,
                          model, 
                          f_mono,
                          p_abs,
                          t_abs,
                          vmr,
                          n2_abs );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "O2-v1v0CKDMT100"==name )
    {
      // Model reference:
      //   Mlawer, Clough, Brown, Stephen, Landry, Goldman, Murcray,
      //   "Observed  Atmospheric Collision Induced Absorption in Near Infrared Oxygen Bands",
      //   Journal of Geophysical Research, vol 103, no. D4, pp. 3859-3863, 1998.
      //
      //  specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT
      //     parameters[0] : continuum scaling
      //     model         : model option ("CKD" or "user")
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     vmr           : [1]
      //     n2_abs        : [1]
      //     h2o_abs       : [1]
      //
      const int Nparam = 1;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          CKD_mt_v1v0_o2( xsec,
                          parameters[0],
                          model, 
                          f_mono,
                          p_abs,
                          t_abs,
                          vmr );
        }  
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          CKD_mt_v1v0_o2( xsec,
                          0.0e0,
                          model, 
                          f_mono,
                          p_abs,
                          t_abs,
                          vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "O2-SelfContStandardType"==name )
    {
      // MPM93, Rosenkranz 1993 O2 continuum:
      // see publication side of National Telecommunications and Information Administration
      //   http://www.its.bldrdoc.gov/pub/all_pubs/all_pubs.html
      // and ftp side for downloading the MPM93 original source code:
      //   ftp://ftp.its.bldrdoc.gov/pub/mpm93/
      //
      // P. W. Rosenkranz Chapter 2, pp 74, in M. A. Janssen, 
      // "Atmospheric Remote Sensing by Microwave Radiometry",
      // John Wiley & Sons, Inc., 1993, ISBN 0-471-62891-3
      // (see also JQSRT, Vol.48, No.5/6 pp.629-643, 1992)
      //
      //  specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT
      //     parameters[0] : continuum coefficient (C)    [1/m*1/Hz*1/Pa] 
      //     parameters[1] : frequency coefficient (G0)   [Hz/Pa]
      //     parameters[3] : line width parameter  (G0A)  [1]
      //     parameters[3] : line width parameter  (G0B)  [1]
      //     parameters[2] : temperature exponent  (XG0d) [1]
      //     parameters[2] : temperature exponent  (x_s)  [1]
      //     parameters[5] : continuum coefficient (XG0w) [1]
      //     model   : model option ("MPM93", "Rosenkranz", or "user")
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     h2o_abs       : [1]
      //     vmr           : [1]
      //
      const int Nparam = 6;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          Standard_O2_continuum( xsec,
                                 parameters[0],
                                 parameters[1], 
                                 parameters[2], 
                                 parameters[3], 
                                 parameters[4], 
                                 parameters[5], 
                                 model, 
                                 f_mono,
                                 p_abs,
                                 t_abs,
                                 h2o_abs,
                                 vmr );
        }  
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          Standard_O2_continuum( xsec,
                                 0.00,
                                 0.00,
                                 0.00,
                                 0.00,
                                 0.00,
                                 0.00,
                                 model, 
                                 f_mono,
                                 p_abs,
                                 t_abs,
                                 h2o_abs,
                                 vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "O2-SelfContMPM93"==name )
    {
      // MPM93 O2 continuum:
      // see publication side of National Telecommunications and Information Administration
      //   http://www.its.bldrdoc.gov/pub/all_pubs/all_pubs.html
      // and ftp side for downloading the MPM93 original source code:
      //   ftp://ftp.its.bldrdoc.gov/pub/mpm93/

      //
      //  specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT
      //     parameters[0] : continuum coefficient (C)    [1/m / (Hz²*Pa²)]
      //     parameters[1] : temperature exponent  (x_s)  [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     h2o_abs       : [1]
      //     vmr           : [1]
      //
      const int Nparam = 4;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          MPM93_O2_continuum( xsec,
                              parameters[0],
                              parameters[1], 
                              parameters[2], 
                              parameters[3], 
                              model, 
                              f_mono,
                              p_abs,
                              t_abs,
                              h2o_abs,
                              vmr );
        }  
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          MPM93_O2_continuum( xsec,
                              0.00,
                              0.00,
                              0.00,
                              0.00,
                              model, 
                              f_mono,
                              p_abs,
                              t_abs,
                              h2o_abs,
                              vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "O2-SelfContPWR93"==name )
    {
      // data information about this continuum: 
      // P. W. Rosenkranz Chapter 2, pp 74, in M. A. Janssen, 
      // "Atmospheric Remote Sensing by Microwave Radiometry",
      // John Wiley & Sons, Inc., 1993, ISBN 0-471-62891-3
      // (see also JQSRT, Vol.48, No.5/6 pp.629-643, 1992)
      // 
      //  specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT
      //     parameters[0] : continuum coefficient (C) [K²/(Hz*Pa*m)]
      //     parameters[1] : temperature exponent  (x) [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     vmr           : [1]
      //
      const int Nparam = 4;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          Rosenkranz_O2_continuum( xsec,
                                   parameters[0],
                                   parameters[1],
                                   parameters[2],
                                   parameters[3],
                                   model,
                                   f_mono,
                                   p_abs,
                                   t_abs,
                                   h2o_abs,
                                   vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          Rosenkranz_O2_continuum( xsec,
                                   0.00,
                                   0.00,
                                   0.00,
                                   0.00,
                                   model,
                                   f_mono,
                                   p_abs,
                                   t_abs,
                                   h2o_abs,
                                   vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ============= O2 full model ========================================================
  else if ( "O2-PWR88"==name )
    {
      //  REFERENCE FOR EQUATIONS AND COEFFICIENTS:
      //  P.W. ROSENKRANZ, CHAP. 2 AND APPENDIX, IN ATMOSPHERIC REMOTE SENSING
      //  BY MICROWAVE RADIOMETRY (M.A. JANSSEN, ED. 1993)
      //  AND 
      //  H.J. LIEBE ET AL, JQSRT V.48, PP.629-643 (1992)
      //  (EXCEPT: SUBMILLIMETER LINE INTENSITIES FROM HITRAN92)
      //  AND
      //  P. W. ROSENKRANZ, INTERFERENCE COEFFICIENTS FOR THE 
      //  OVERLAPPING OXYGEN LINES IN AIR, JQSRT, 1988, VOLUME 39, 287-297.
      //
      //  the only difference to the 1993 version is the line mixing 
      //  parameter Y, which is taken from the above reference JQSRT, 1988.
      //
      //  specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT
      //     parameters[0] : continuum term scale factor,   default CC = 1.000 [1]
      //     parameters[1] : line strength scale factor,    default CL = 1.000 [1]
      //     parameters[1] : line broadening scale factor,  default CW = 1.000 [1]
      //     parameters[1] : line coupling scale factor,    default CO = 1.000 [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     h2o_abs,      : [1]
      //     vmr           : [1]
      //
      const int Nparam = 4;
      const char *version="PWR88";
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Full model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          PWR93O2AbsModel( xsec,
                           parameters[0], // continuum term scale factor
                           parameters[1], // line strength scale factor
                           parameters[2], // line broadening scale factor
                           parameters[3], // line coupling scale factor
                           model,
                           version, 
                           f_mono,
                           p_abs,
                           t_abs,
                           h2o_abs,
                           vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Full model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Full model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          PWR93O2AbsModel( xsec,
                           0.00,
                           0.00,
                           0.00,
                           0.00,
                           model,
                           version,
                           f_mono,
                           p_abs,
                           t_abs,
                           h2o_abs,
                           vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Full model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "O2-PWR93"==name )
    {
      //  REFERENCE FOR EQUATIONS AND COEFFICIENTS:
      //  P.W. ROSENKRANZ, CHAP. 2 AND APPENDIX, IN ATMOSPHERIC REMOTE SENSING
      //  BY MICROWAVE RADIOMETRY (M.A. JANSSEN, ED. 1993)
      //  AND H.J. LIEBE ET AL, JQSRT V.48, PP.629-643 (1992)
      //  (EXCEPT: SUBMILLIMETER LINE INTENSITIES FROM HITRAN92)
      //
      //  specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT
      //     parameters[0] : continuum term scale factor,   default CC = 1.000 [1]
      //     parameters[1] : line strength scale factor,    default CL = 1.000 [1]
      //     parameters[1] : line broadening scale factor,  default CW = 1.000 [1]
      //     parameters[1] : line coupling scale factor,    default CO = 1.000 [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     h2o_abs,      : [1]
      //     vmr           : [1]
      //
      const int Nparam = 4;
      const char *version="PWR93";
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Full model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          PWR93O2AbsModel( xsec,
                           parameters[0], // continuum term scale factor
                           parameters[1], // line strength scale factor
                           parameters[2], // line broadening scale factor
                           parameters[3], // line coupling scale factor
                           model,
                           version,
                           f_mono,
                           p_abs,
                           t_abs,
                           h2o_abs,
                           vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Full model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Full model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          PWR93O2AbsModel( xsec,
                           0.00,
                           0.00,
                           0.00,
                           0.00,
                           model,
                           version,
                           f_mono,
                           p_abs,
                           t_abs,
                           h2o_abs,
                           vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Full model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "O2-PWR98"==name )
    {
      //  REFERENCES FOR EQUATIONS AND COEFFICIENTS:
      //    P.W. Rosenkranz, CHAP. 2 and appendix, in ATMOSPHERIC REMOTE SENSING
      //     BY MICROWAVE RADIOMETRY (M.A. Janssen, ed., 1993).
      //    H.J. Liebe et al, JQSRT V.48, PP.629-643 (1992).
      //    M.J. Schwartz, Ph.D. thesis, M.I.T. (1997).
      //    SUBMILLIMETER LINE INTENSITIES FROM HITRAN96.
      //    This version differs from Liebe's MPM92 in two significant respects:
      //    1. It uses the modification of the 1- line width temperature dependence
      //    recommended by Schwartz: (1/T).
      //    2. It uses the same temperature dependence (X) for submillimeter 
      //    line widths as in the 60 GHz band: (1/T)**0.8 
      //
      //  specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT
      //     parameters[0] : continuum term scale factor,   default CC = 1.000 [1]
      //     parameters[1] : line strength scale factor,    default CL = 1.000 [1]
      //     parameters[1] : line broadening scale factor,  default CW = 1.000 [1]
      //     parameters[1] : line coupling scale factor,    default CO = 1.000 [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     h2o_abs,      : [1]
      //     vmr           : [1]
      //
      const int Nparam = 4;
      const char *version="PWR98";
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Full model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          PWR93O2AbsModel( xsec,
                           parameters[0], // continuum term scale factor
                           parameters[1], // line strength scale factor
                           parameters[2], // line broadening scale factor
                           parameters[3], // line coupling scale factor
                           model,
                           version, 
                           f_mono,
                           p_abs,
                           t_abs,
                           h2o_abs,
                           vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Full model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Full model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          PWR93O2AbsModel( xsec,
                           0.00,
                           0.00,
                           0.00,
                           0.00,
                           model,
                           version,
                           f_mono,
                           p_abs,
                           t_abs,
                           h2o_abs,
                           vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Full model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "O2-MPM93"==name )
    {
      //  H. J. Liebe and G. A. Hufford and M. G. Cotton,
      //  "Propagation modeling of moist air and suspended water/ice
      //   particles at frequencies below 1000 GHz",
      //  AGARD 52nd Specialists Meeting of the Electromagnetic Wave
      //  Propagation Panel, Palma de Mallorca, Spain, 1993, May 17-21       
      //
      //  specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT
      //     parameters[0] : continuum term scale factor,   default CC = 1.000 [1]
      //     parameters[1] : line strength scale factor,    default CL = 1.000 [1]
      //     parameters[2] : line broadening scale factor,  default CW = 1.000 [1]
      //     parameters[3] : line coupling scale factor,    default CO = 1.000 [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     h2o_abs,      : [1]
      //     vmr           : [1]
      //
      const int Nparam = 4;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Full model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          MPM93O2AbsModel( xsec,
                           parameters[0], // continuum term scale factor
                           parameters[1], // line strength scale factor
                           parameters[2], // line broadening scale factor
                           parameters[3], // line coupling scale factor
                           model,
                           f_mono,
                           p_abs,
                           t_abs,
                           h2o_abs,
                           vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Full model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Full model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          MPM93O2AbsModel( xsec,
                           0.00,
                           0.00,
                           0.00,
                           0.00,
                           model,
                           f_mono,
                           p_abs,
                           t_abs,
                           h2o_abs,
                           vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Full model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "O2-MPM92"==name )
    {
      //   H. J. Liebe, P. W. Rosenkranz and G. A. Hufford,
      //   Atmospheric 60-GHz Oxygen Spectrum: New Laboratory 
      //   Measurements and Line Parameters
      //   JQSRT, Vol 48, pp. 629-643, 1992
      //
      //  specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT
      //     parameters[0] : continuum term scale factor,   default CC = 1.000 [1]
      //     parameters[1] : line strength scale factor,    default CL = 1.000 [1]
      //     parameters[2] : line broadening scale factor,  default CW = 1.000 [1]
      //     parameters[3] : line coupling scale factor,    default CO = 1.000 [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     h2o_abs,      : [1]
      //     vmr           : [1]
      //
      const int Nparam = 4;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Full model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          MPM92O2AbsModel( xsec,
                           parameters[0], // continuum term scale factor
                           parameters[1], // line strength scale factor
                           parameters[2], // line broadening scale factor
                           parameters[3], // line coupling scale factor
                           model,
                           f_mono,
                           p_abs,
                           t_abs,
                           h2o_abs,
                           vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Full model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Full model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          MPM92O2AbsModel( xsec,
                           0.00,
                           0.00,
                           0.00,
                           0.00,
                           model,
                           f_mono,
                           p_abs,
                           t_abs,
                           h2o_abs,
                           vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Full model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "O2-MPM89"==name )
    {
      //   H. J. Liebe,
      //   MPM - an atmospheric millimeter-wave propagation model,
      //   Int. J. Infrared and Mill. Waves, Vol 10, pp. 631-650, 1989.
      //
      //  specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT
      //     parameters[0] : continuum term scale factor,   default CC = 1.000 [1]
      //     parameters[1] : line strength scale factor,    default CL = 1.000 [1]
      //     parameters[2] : line broadening scale factor,  default CW = 1.000 [1]
      //     parameters[3] : line coupling scale factor,    default CO = 1.000 [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     h2o_abs,      : [1]
      //     vmr           : [1]
      //
      const int Nparam = 4;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Full model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          MPM89O2AbsModel( xsec,
                           parameters[0], // continuum term scale factor
                           parameters[1], // line strength scale factor
                           parameters[2], // line broadening scale factor
                           parameters[3], // line coupling scale factor
                           model,
                           f_mono,
                           p_abs,
                           t_abs,
                           h2o_abs,
                           vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Full model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Full model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          MPM89O2AbsModel( xsec,
                           0.00,
                           0.00,
                           0.00,
                           0.00,
                           model,
                           f_mono,
                           p_abs,
                           t_abs,
                           h2o_abs,
                           vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Full model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "O2-MPM87"==name )
    {
      //   H. J. Liebe and D. H. Layton,
      //   Millimeter-wave properties of the atmosphere: 
      //   Laboratory studies and propagation modelling,
      //   NITA Report 87-224, 
      //   U.S. Dept. of Commerce, National Telecommunications and Information
      //   Administration, Institute for Communication Sciences, rep. 87-224,
      //   325 Broadway, Boulder, CO 80303-3328
      //
      //  specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT
      //     parameters[0] : continuum term scale factor,   default CC = 1.000 [1]
      //     parameters[1] : line strength scale factor,    default CL = 1.000 [1]
      //     parameters[2] : line broadening scale factor,  default CW = 1.000 [1]
      //     parameters[3] : line coupling scale factor,    default CO = 1.000 [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     h2o_abs,      : [1]
      //     vmr           : [1]
      //
      const int Nparam = 4;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Full model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          MPM87O2AbsModel( xsec,
                           parameters[0], // continuum term scale factor
                           parameters[1], // line strength scale factor
                           parameters[2], // line broadening scale factor
                           parameters[3], // line coupling scale factor
                           model,
                           f_mono,
                           p_abs,
                           t_abs,
                           h2o_abs,
                           vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Full model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Full model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          MPM87O2AbsModel( xsec,
                           0.00,
                           0.00,
                           0.00,
                           0.00,
                           model,
                           f_mono,
                           p_abs,
                           t_abs,
                           h2o_abs,
                           vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Full model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "O2-MPM85"==name )
    {
      //   H. J. Liebe and D. H. Layton,
      //   An updated model for millimeter wave propagation in moist air
      //   Radio Science, vol. 20, pp. 1069-1089, 1985
      //
      //  specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT
      //     parameters[0] : continuum term scale factor,   default CC = 1.000 [1]
      //     parameters[1] : line strength scale factor,    default CL = 1.000 [1]
      //     parameters[2] : line broadening scale factor,  default CW = 1.000 [1]
      //     parameters[3] : line coupling scale factor,    default CO = 1.000 [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     h2o_abs,      : [1]
      //     vmr           : [1]
      //
      const int Nparam = 4;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Full model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          MPM85O2AbsModel( xsec,
                           parameters[0], // continuum term scale factor
                           parameters[1], // line strength scale factor
                           parameters[2], // line broadening scale factor
                           parameters[3], // line coupling scale factor
                           model,
                           f_mono,
                           p_abs,
                           t_abs,
                           h2o_abs,
                           vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Full model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Full model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          MPM85O2AbsModel( xsec,
                           0.00,
                           0.00,
                           0.00,
                           0.00,
                           model,
                           f_mono,
                           p_abs,
                           t_abs,
                           h2o_abs,
                           vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Full model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ============= N2 continuum =========================================================
  else if ( "N2-SelfContMPM93"==name )
    {
      // MPM93 N2 continuum:
      // see publication side of National Telecommunications and Information Administration
      //   http://www.its.bldrdoc.gov/pub/all_pubs/all_pubs.html
      // and ftp side for downloading the MPM93 original source code:
      //   ftp://ftp.its.bldrdoc.gov/pub/mpm93/
      //
      //  specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT
      //     parameters[0] : strength parameter   [1/m * 1/(Hz²*Pa²)]
      //     parameters[1] : broadening parameter [1]
      //     parameters[2] : temperature exponent [1]
      //     parameters[3] : frequency exponent   [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     h2o_abs       : [1]
      //     vmr           : [1]
      //
      const int Nparam = 4;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          MPM93_N2_continuum( xsec,
                              parameters[0],
                              parameters[1],
                              parameters[2],                      
                              parameters[3],                      
                              model,
                              f_mono,
                              p_abs,
                              t_abs,
                              h2o_abs,
                              vmr );
        }  
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model == "MPM93Scale") && (parameters.nelem() == 1) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          MPM93_N2_continuum( xsec,
                              parameters[0],
                              0.00,
                              0.00,
                              0.00,
                              model,
                              f_mono,
                              p_abs,
                              t_abs,
                              h2o_abs,
                              vmr );
        }
      else if ( (model == "MPM93Scale") && (parameters.nelem() != 1) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires 1 scaling input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (model != "MPM93Scale") && (parameters.nelem() == 0) ) // --
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          MPM93_N2_continuum( xsec,
                              0.00,
                              0.00,
                              0.00,
                              0.00,
                              model,
                              f_mono,
                              p_abs,
                              t_abs,
                              h2o_abs,
                              vmr );
        }
      /* --------------------------------------------------------------------------
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
      ----------------------------------------------------------------------*/
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "N2-DryContATM01"==name )
    {
      // data information about this continuum: 
      // Pardo et al. model model (IEEE, Trans. Ant. Prop., 
      // Vol 49, No 12, pp. 1683-1694, 2001)
      //
      // specific continuum parameters and units:
      //  a) output 
      //     xsec          : [1/m],
      //  b) input
      //     parameters[0] : continuum strength coefficient  [1/m * 1/(Hz*Pa)²]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     vmr           : [1]   for  N2
      //     h2ovmr        : [1]   for  H2O
      //
      const int Nparam = 1;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          Pardo_ATM_N2_dry_continuum( xsec,
                                      parameters[0], // coefficient
                                      model,
                                      f_mono,
                                      p_abs,
                                      t_abs,
                                      vmr,
                                      h2o_abs );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          Pardo_ATM_N2_dry_continuum( xsec,
                                      0.000, // coefficient
                                      model,
                                      f_mono,
                                      p_abs,
                                      t_abs,
                                      vmr,
                                      h2o_abs );
        } 
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "N2-SelfContPWR93"==name )
    {
      // data information about this continuum: 
      // P. W. Rosenkranz Chapter 2, pp 74, in M. A. Janssen, 
      // "Atmospheric Remote Sensing by Microwave Radiometry",
      // John Wiley & Sons, Inc., 1993, ISBN 0-471-62891-3
      //
      // specific continuum parameters and units:
      //  a) output 
      //     xsec          : [1/m],
      //  b) input
      //     parameters[0] : continuum strength coefficient  [1/m * 1/(Hz*Pa)²]
      //     parameters[1] : continuum temperature exponent  [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     vmr           : [1]
      //
      const int Nparam = 2;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          Rosenkranz_N2_self_continuum( xsec,
                                        parameters[0], // coefficient
                                        parameters[1], // temp. exponent
                                        model,
                                        f_mono,
                                        p_abs,
                                        t_abs,
                                        vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          Rosenkranz_N2_self_continuum( xsec,
                                        0.00,
                                        0.00,
                                        model,
                                        f_mono,
                                        p_abs,
                                        t_abs,
                                        vmr );    
        } 
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "N2-SelfContStandardType"==name )
    {
      // data information about this continuum: 
      // A completely general expression for the N2 continuum
      //
      // specific continuum parameters and units:
      // OUTPUT 
      //     xsec          : [1/m],
      // INPUT
      //     parameters[0] : continuum coefficient (C)  [1/m * 1/(Hz*Pa)²]
      //     parameters[1] : frequency exponent    (xf) [1]
      //     parameters[2] : temperature exponent  (xt) [1]
      //     parameters[3] : pressure exponent     (xp) [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     vmr           : [1]
      const int Nparam = 4;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          Standard_N2_self_continuum( xsec,
                                      parameters[0],
                                      parameters[1],
                                      parameters[2],
                                      parameters[3],
                                      model,
                                      f_mono,
                                      p_abs,
                                      t_abs,
                                      vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          Standard_N2_self_continuum( xsec,
                                      0.000,
                                      0.000,
                                      0.000,
                                      0.000,
                                      model,
                                      f_mono,
                                      p_abs,
                                      t_abs,
                                      vmr );
        } 
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }  
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "N2-SelfContBorysow"==name )
    {
      // data information about this continuum: 
      // A. Borysow and L. Frommhold, The Astrophysical Journal,
      // Vol. 311, pp.1043-1057, 1986
      const int Nparam = 1;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          BF86_CIA_N2( xsec,
                       parameters[0], // scaling factor
                       model,
                       f_mono,
                       p_abs,
                       t_abs,
                       vmr   );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          BF86_CIA_N2( xsec,
                       0.0,
                       model,
                       f_mono,
                       p_abs,
                       t_abs,
                       vmr   );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters. " << "\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }  
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "N2-CIArotCKDMT100"==name )
    {
      // data information about this continuum: 
      // A. Borysow and L. Frommhold, The Astrophysical Journal,
      // Vol. 311, pp.1043-1057, 1986
      const int Nparam = 1;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          CKD_mt_CIArot_n2( xsec,
                            parameters[0], // scaling factor
                            model,
                            f_mono,
                            p_abs,
                            t_abs,
                            vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          CKD_mt_CIArot_n2( xsec,
                            0.0,
                            model,
                            f_mono,
                            p_abs,
                            t_abs,
                            vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters. " << "\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }  
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "N2-CIAfunCKDMT100"==name )
    {
      // data information about this continuum: 
      // Lafferty, W.J., A.M. Solodov,A. Weber, W.B. Olson and J._M. Hartmann,
      // Infrared collision-induced absorption by 
      // N2 near 4.3 microns for atmospheric applications: 
      // Measurements and emprirical modeling,
      // Appl. Optics, 35, 5911-5917, (1996)

      const int Nparam = 1;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          CKD_mt_CIAfun_n2( xsec,
                            parameters[0], // scaling factor
                            model,
                            f_mono,
                            p_abs,
                            t_abs,
                            vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          CKD_mt_CIAfun_n2( xsec,
                            0.0,
                            model,
                            f_mono,
                            p_abs,
                            t_abs,
                            vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters. " << "\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }  
  // ============= CO2 continuum ========================================================
  else if ( "CO2-CKD241"==name )
    {
      // data information about this continuum: 
      // CKDv2.4.1 model at http://www.rtweb.aer.com/continuum_frame.html
      // This continuum accounts for the far wings of the many COS lines/bands since
      // the line is used with a cutoff in the line shape with +/- 25 cm^-1.
      //
      // specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT 
      //     parameters[0] : continuum strength coefficient [1/m * 1/(Hz*Pa)²]
      //     parameters[1] : continuum temperature exponent  [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     vmr           : [1]
      //     h2o_abs       : [1]
      //
      const int Nparam = 1;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          CKD_241_co2( xsec,
                      parameters[0], // abs. scaling
                      model,
                      f_mono,
                      p_abs,
                      t_abs,
                      vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          CKD_241_co2( xsec,
                      0.00,
                      model,
                      f_mono,
                      p_abs,
                      t_abs,
                      vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters. " << "\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "CO2-CKDMT100"==name )
    {
      // data information about this continuum: 
      // CKD model at http://www.rtweb.aer.com/continuum_frame.html
      // This continuum accounts for the far wings of the many COS lines/bands since
      // the line is used with a cutoff in the line shape with +/- 25 cm^-1.
      //
      // specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT 
      //     parameters[0] : continuum strength coefficient [1/m * 1/(Hz*Pa)²]
      //     parameters[1] : continuum temperature exponent  [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     vmr           : [1]
      //     h2o_abs       : [1]
      //
      const int Nparam = 1;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          CKD_mt_co2( xsec,
                      parameters[0], // abs. scaling
                      model,
                      f_mono,
                      p_abs,
                      t_abs,
                      vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          CKD_mt_co2( xsec,
                      0.00,
                      model,
                      f_mono,
                      p_abs,
                      t_abs,
                      vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters. " << "\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "CO2-SelfContPWR93"==name )
    {
      // data information about this continuum: 
      // P. W. Rosenkranz Chapter 2, pp 74, in M. A. Janssen, 
      // "Atmospheric Remote Sensing by Microwave Radiometry",
      // John Wiley & Sons, Inc., 1993, ISBN 0-471-62891-3
      //
      // specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT 
      //     parameters[0] : continuum strength coefficient [1/m * 1/(Hz*Pa)²]
      //     parameters[1] : continuum temperature exponent  [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     vmr           : [1]
      //
      const int Nparam = 2;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          Rosenkranz_CO2_self_continuum( xsec,
                                         parameters[0], // coefficient
                                         parameters[1], // temp. exponent
                                         model,
                                         f_mono,
                                         p_abs,
                                         t_abs,
                                         vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          Rosenkranz_CO2_self_continuum( xsec,
                                         0.00,
                                         0.00,
                                         model,
                                         f_mono,
                                         p_abs,
                                         t_abs,
                                         vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters. " << "\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
  else if ( "CO2-ForeignContPWR93"==name )
    {
      // data information about this continuum: 
      // P. W. Rosenkranz Chapter 2, pp 74, in M. A. Janssen, 
      // "Atmospheric Remote Sensing by Microwave Radiometry",
      // John Wiley & Sons, Inc., 1993, ISBN 0-471-62891-3
      //
      // specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT
      //     parameters[0] : continuum strength coefficient [1/m * 1/(Hz*Pa)²]
      //     parameters[1] : continuum temperature exponent  [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     n2_abs        : [1]
      //     vmr           : [1]
      //
      const int Nparam = 2;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "Continuum model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          Rosenkranz_CO2_foreign_continuum( xsec,
                                            parameters[0],
                                            parameters[1],
                                            model,
                                            f_mono,
                                            p_abs,
                                            t_abs,
                                            n2_abs,
                                            vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "Continuum model " << name << " requires " << Nparam << " input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "Continuum model " << name << " running with \n" 
               << "the parameters for model " << model << ".\n";
          Rosenkranz_CO2_foreign_continuum( xsec,
                                            0.00,
                                            0.00,
                                            model,
                                            f_mono,
                                            p_abs,
                                            t_abs,
                                            n2_abs,
                                            vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: Continuum model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters. " << "\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 3.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ============= cloud and fog absorption from MPM93 ==================================
  else if ( "liquidcloud-MPM93"==name )
    {
      // Suspended water droplet absorption parameterization from MPM93 model
      // H. J. Liebe and G. A. Hufford and M. G. Cotton,
      // "Propagation modeling of moist air and suspended water/ice
      //  particles at frequencies below 1000 GHz",
      // AGARD 52nd Specialists Meeting of the Electromagnetic Wave
      // Propagation Panel, Palma de Mallorca, Spain, 1993, May 17-21 
      //
      // specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT 
      //     parameters[0] : [1]
      //     parameters[1] : [1]
      //     parameters[2] : [1]
      //     model        : [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     vmr           : [1]
      //
      // liquid water droplet parameters:
      // suspended water droplet density   range: 0-10 g/m³
      // specific droplet weight           value:    1 g/cm³
      //
      // valid atmospheric condition:
      // temperature      : 233 to 323 K
      // relative humidity:   1 to 100 %
      // 
      const int Nparam = 3;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "MPM93 liquid water cloud absorption model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          MPM93WaterDropletAbs(xsec,
                               parameters[0],     // scaling factror
                               parameters[1],     // scaling factror
                               parameters[2],     // scaling factror
                               model,       // model option
                               f_mono,
                               p_abs,
                               t_abs,
                               vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "MPM93 liquid water cloud absorption model " << name << " requires\n" 
             << Nparam << " input parameter for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "MPM93 liquid water cloud absorption model " << name << " running with \n" 
               << "the parameter for model " << model << ".\n";
          MPM93WaterDropletAbs(xsec,
                               0.000,        // scaling factror
                               0.000,        // scaling factror
                               0.000,        // scaling factror
                               model,  // model option
                               f_mono,
                               p_abs,
                               t_abs,
                               vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: MPM93 liquid water cloud absorption model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 4.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ============= ice particle absorption from MPM93 ===================================
  else if ( "icecloud-MPM93"==name )
    {
      // Ice particle absorption parameterization from MPM93 model
      // H. J. Liebe and G. A. Hufford and M. G. Cotton,
      // "Propagation modeling of moist air and suspended water/ice
      //  particles at frequencies below 1000 GHz",
      // AGARD 52nd Specialists Meeting of the Electromagnetic Wave
      // Propagation Panel, Palma de Mallorca, Spain, 1993, May 17-21 
      //
      // specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT 
      //     parameters[0] : [1]
      //     parameters[1] : [1]
      //     parameters[2] : [1]
      //     model        : [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     vmr           : [1]
      //
      // ice crystal parameters:
      // suspended water droplet density   range: 0-10 g/m³
      // specific droplet weight           value:    1 g/cm³
      //
      // valid atmospheric condition:
      // temperature      : 233 to 323 K
      // relative humidity:   1 to 100 %
      // 
      const int Nparam = 3;
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "MPM93 ice water cloud absorption model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          MPM93IceCrystalAbs(xsec,
                             parameters[0],     // scaling factror
                             parameters[1],     // scaling factror
                             parameters[2],     // scaling factror
                             model,       // model option
                             f_mono,
                             p_abs,
                             t_abs,
                             vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "MPM93 ice water cloud absorption model " << name << " requires \n"
             << Nparam << " input parameter for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "MPM93 ice water cloud absorption model " << name << " running with \n" 
               << "the parameter for model " << model << ".\n";
          MPM93IceCrystalAbs(xsec,
                             0.000,       // scaling factror
                             0.000,       // scaling factror
                             0.000,       // scaling factror
                             model, // model option
                             f_mono,
                             p_abs,
                             t_abs,
                             vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: MPM93 ice water cloud absorption model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 4.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  // ============= rain extinction from MPM93 ===========================================
  else if ( "rain-MPM93"==name )
    {
      // Rain extinction parameterization from MPM93 model, described in
      //  H. J. Liebe, 
      //  "MPM - An Atmospheric Millimeter-Wave Propagation Model",
      //  Int. J. Infrared and Millimeter Waves, vol. 10(6),
      //  pp. 631-650, 1989
      // and based on 
      //  Olsen, R.L., D.V. Rogers, and D. B. Hodge, "The aR^b relation in the
      //  calculation of rain attenuation", IEEE Trans. Antennas Propagat.,
      // vol. AP-26, pp. 318-329, 1978.
      //
      // specific continuum parameters and units:
      //  OUTPUT 
      //     xsec          : [1/m],
      //  INPUT 
      //     parameters[0] : [1]
      //     parameters[1] : [1]
      //     parameters[2] : [1]
      //     model         : [1]
      //     f_mono        : [Hz]
      //     p_abs         : [Pa]
      //     t_abs         : [K]
      //     vmr           : [mm/h]
      //
      // rain parameters:
      // rain rate                         range: 0-150 mm/h
      //
      // valid atmospheric condition:
      // temperature      : (preferably above 273 K...)
      // 
      const int Nparam = 3; 
      if ( (model == "user") && (parameters.nelem() == Nparam) ) // -------------------------
        {
          out3 << "MPM93 rain extinction model " << name << " is running with \n"
               << "user defined parameters according to model " << model << ".\n";
          MPM93RainExt(xsec,
                       parameters[0],     // scaling factror
                       parameters[1],     // scaling factror
                       parameters[2],     // scaling factror
                       model,             // model option
                       f_mono,
                       p_abs,
                       t_abs,
                       vmr );
        }
      else if ( (model == "user") && (parameters.nelem() != Nparam) ) // --------------------
        {
          ostringstream os;
          os << "MPM93 rain extinction model  " << name << " requires \n"
             << Nparam << " input parameter for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n";
          throw runtime_error(os.str());
          return;
        }
      else if ( (model != "user") && (parameters.nelem() == 0) ) // --------------------
        {
          out3 << "MPM93 rain extinction model " << name << " running with \n" 
               << "the parameter for model " << model << ".\n";
         MPM93RainExt(xsec,
                      0.000,       // scaling factror
                      0.000,       // scaling factror
                      0.000,       // scaling factror
                      model,       // model option
                      f_mono,
                      p_abs,
                      t_abs,
                      vmr );
        }
      else if ( (model != "user") && (parameters.nelem() != 0) ) // --------------------
        {
          ostringstream os;
          os << "ERROR: MPM93 rain extinction model " << name << " requires NO input\n"
             << "parameters for the model " << model << ",\n"
             << "but you specified " << parameters.nelem() << " parameters.\n"
             << "This ambiguity can not be solved by arts.\n"
             << "Please see the arts user guide chapter 4.\n";
          throw runtime_error(os.str());
          return;
        }
    }
  else // -----------------------------------------------------------------------
    {
      // none of the continuum or full model tags were selected -> error message.
      ostringstream os;
      os << "ERROR: Continuum/ full model tag `" << name << "' not yet implemented in arts!";
      throw runtime_error(os.str());
      return;
    }
 return;
}
//
// #################################################################################
//
void check_continuum_model(const String& name)
{
  // The species lookup data:
  extern const Array<SpeciesRecord> species_data;

  // For the list of valid continuum models:
  ArrayOfString valid_models;

  bool found = false;

  // Loop all species:
  for ( Array<SpeciesRecord>::const_iterator i=species_data.begin();
        i<species_data.end();
        ++i )
    {
      String specnam = i->Name();

      // Loop all isotopes:
      for ( Array<IsotopeRecord>::const_iterator j=i->Isotope().begin();
            j<i->Isotope().end();
            ++j )
        {
          String isonam = j->Name();

          // The specified name consists of a species part and an
          // isotope part, e.g., H2O-ContStandardSelf. We need to
          // construct a similar String from the species lookup data
          // by concatenating species name and isotope name.

          String fullnam = specnam + "-" + isonam;
          //      cout << fullnam << "\n";

          // See if this is a continuum tag, so that we can add it to
          // the list:
          if ( 0 > j->Abundance() )
            {
              valid_models.push_back(fullnam);        
            }
          
          if ( name == fullnam )
            {
              found = true;
            }
        }
    }

  // ----------------------------------------------------------------------
  // Have we found it?
  if (!found)
    {
      ostringstream os;
      os << "The String `" << name << "' matches none of the known\n"
         << "continuum models. Known continuum models are:";
      for ( ArrayOfString::const_iterator i=valid_models.begin();
            i<valid_models.end();
            ++i )
        {
          os << "\n" << *i;
        }      
      throw runtime_error(os.str());
    }
}
//
//
// #################################################################################
// ############################# f2c code implementation ###########################
// #################################################################################
//
//
// ------------------- begin of f2c.h file --------------------------------
//
/* f2c.h  --  Standard Fortran to C header file */
#ifndef F2C_INCLUDE
#define F2C_INCLUDE

typedef long int integer;
typedef unsigned long int uinteger;
typedef char *address;
typedef short int shortint;
typedef float real;
typedef double doublereal;
typedef struct { real r, i; } complex;
typedef struct { doublereal r, i; } doublecomplex;
typedef long int logical;
typedef short int shortlogical;
typedef char logical1;
typedef char integer1;
#ifdef INTEGER_STAR_8   /* Adjust for integer*8. */
typedef long long longint;              /* system-dependent */
typedef unsigned long long ulongint;    /* system-dependent */
#define qbit_clear(a,b) ((a) & ~((ulongint)1 << (b)))
#define qbit_set(a,b)   ((a) |  ((ulongint)1 << (b)))
#endif

#define TRUE_ (1)
#define FALSE_ (0)

/* Extern is for use with -E */
#ifndef Extern
#define Extern extern
#endif

/* I/O stuff */

#ifdef f2c_i2
/* for -i2 */
typedef short flag;
typedef short ftnlen;
typedef short ftnint;
#else
typedef long int flag;
typedef long int ftnlen;
typedef long int ftnint;
#endif

/*external read, write*/
typedef struct
{       flag cierr;
        ftnint ciunit;
        flag ciend;
        char *cifmt;
        ftnint cirec;
} cilist;

/*internal read, write*/
typedef struct
{       flag icierr;
        char *iciunit;
        flag iciend;
        char *icifmt;
        ftnint icirlen;
        ftnint icirnum;
} icilist;

/*open*/
typedef struct
{       flag oerr;
        ftnint ounit;
        char *ofnm;
        ftnlen ofnmlen;
        char *osta;
        char *oacc;
        char *ofm;
        ftnint orl;
        char *oblnk;
} olist;

/*close*/
typedef struct
{       flag cerr;
        ftnint cunit;
        char *csta;
} cllist;

/*rewind, backspace, endfile*/
typedef struct
{       flag aerr;
        ftnint aunit;
} alist;

/* inquire */
typedef struct
{       flag inerr;
        ftnint inunit;
        char *infile;
        ftnlen infilen;
        ftnint  *inex;  /*parameters in standard's order*/
        ftnint  *inopen;
        ftnint  *innum;
        ftnint  *innamed;
        char    *inname;
        ftnlen  innamlen;
        char    *inacc;
        ftnlen  inacclen;
        char    *inseq;
        ftnlen  inseqlen;
        char    *indir;
        ftnlen  indirlen;
        char    *infmt;
        ftnlen  infmtlen;
        char    *inform;
        ftnint  informlen;
        char    *inunf;
        ftnlen  inunflen;
        ftnint  *inrecl;
        ftnint  *innrec;
        char    *inblank;
        ftnlen  inblanklen;
} inlist;

#define VOID void

union Multitype {       /* for multiple entry points */
        integer1 g;
        shortint h;
        integer i;
        /* longint j; */
        real r;
        doublereal d;
        complex c;
        doublecomplex z;
        };

typedef union Multitype Multitype;

/*typedef long int Long;*/      /* No longer used; formerly in Namelist */

struct Vardesc {        /* for Namelist */
        char *name;
        char *addr;
        ftnlen *dims;
        int  type;
        };
typedef struct Vardesc Vardesc;

struct Namelist {
        char *name;
        Vardesc **vars;
        int nvars;
        };
typedef struct Namelist Namelist;

#define abs(x) ((x) >= 0 ? (x) : -(x))
#define dabs(x) (doublereal)abs(x)
#define min(a,b) ((a) <= (b) ? (a) : (b))
#define max(a,b) ((a) >= (b) ? (a) : (b))
#define dmin(a,b) (doublereal)min(a,b)
#define dmax(a,b) (doublereal)max(a,b)
#define bit_test(a,b)   ((a) >> (b) & 1)
#define bit_clear(a,b)  ((a) & ~((uinteger)1 << (b)))
#define bit_set(a,b)    ((a) |  ((uinteger)1 << (b)))

/* procedure parameter types for -A and -C++ */

#define F2C_proc_par_types 1
#ifdef __cplusplus
typedef int /* Unknown procedure type */ (*U_fp)(...);
typedef shortint (*J_fp)(...);
typedef integer (*I_fp)(...);
typedef real (*R_fp)(...);
typedef doublereal (*D_fp)(...), (*E_fp)(...);
typedef /* Complex */ VOID (*C_fp)(...);
typedef /* Double Complex */ VOID (*Z_fp)(...);
typedef logical (*L_fp)(...);
typedef shortlogical (*K_fp)(...);
typedef /* Character */ VOID (*H_fp)(...);
typedef /* Subroutine */ int (*S_fp)(...);
#else
typedef int /* Unknown procedure type */ (*U_fp)();
typedef shortint (*J_fp)();
typedef integer (*I_fp)();
typedef real (*R_fp)();
typedef doublereal (*D_fp)(), (*E_fp)();
typedef /* Complex */ VOID (*C_fp)();
typedef /* Double Complex */ VOID (*Z_fp)();
typedef logical (*L_fp)();
typedef shortlogical (*K_fp)();
typedef /* Character */ VOID (*H_fp)();
typedef /* Subroutine */ int (*S_fp)();
#endif
/* E_fp is for real functions when -R is not specified */
typedef VOID C_f;       /* complex function */
typedef VOID H_f;       /* character function */
typedef VOID Z_f;       /* double complex function */
typedef doublereal E_f; /* real function with -R not specified */

/* undef any lower-case symbols that your C compiler predefines, e.g.: */

#ifndef Skip_f2c_Undefs
#undef cray
#undef gcos
#undef mc68010
#undef mc68020
#undef mips
#undef pdp11
#undef sgi
#undef sparc
#undef sun
#undef sun2
#undef sun3
#undef sun4
#undef u370
#undef u3b
#undef u3b2
#undef u3b5
#undef unix
#undef vax
#endif
#endif

// ------------------- end of f2c.h file --------------------------------


// ------------------ begin of Borysow N2N2 F77 code --------------------


/* n2n2tks.f -- translated by f2c (version 20010821).
   You must link the resulting object file with the libraries:
        -lf2c -lm   (in that order)
*/

/* Common Block Declarations */

struct s_blockin_ {
    double temp, fnumin, fnumax, dnu;
} blockin_;

#define blockin_1 blockin_

struct s_app3a_ {
    double slit, dx, wnrmax3;
} app3a_;

#define app3a_1 app3a_

struct s_app3b_ {
    int nsri, ns, nsriup;
} app3b_;

#define app3b_1 app3b_

struct s_rsilo_ {
    double rsilo[201];
} rsilo_;

#define rsilo_1 rsilo_

struct s_bou43_ {
    int initb;
} bou43_;

#define bou43_1 bou43_

union u_bba_ {
    struct s_m_1 {
        double omeg[201], rsi[201], rsigg[201], alfa;
    } m_1;
    struct s_m_2 {
        double omeg[201], rsi[201], rsigg[201], beta;
    } m_2;
} bba_;

#define bba_1 (bba_.m_1)
#define bba_2 (bba_.m_2)

struct s_bbc_ {
    int nsol;
} bbc_;

#define bbc_1 bbc_

struct s_bf_ {
    double g0bf, delbf, om0;
} bf_;

#define bf_1 bf_

struct like_1_ {
    int like;
    char lgas[5];
};

#define like_1 (*(struct like_1_ *) &like_)

struct s_k1k0_ {
    int ik1k0;
} k1k0_;

#define k1k0_1 k1k0_

struct s_bbb_ {
    int ibound;
} bbb_;

#define bbb_1 bbb_

struct energ_1_ {
    double eb[246]      /* was [41][6] */;
    int niv[6];
};

#define energ_1 (*(struct energ_1_ *) &energ_)

struct s_dimer_ {
    int nlines;
} dimer_;

#define dimer_1 dimer_

struct n2part_1_ {
    double q1, wn2[2], b01, d01;
    int jrange2;
};
struct n2part_2_ {
    double q, wn2[2], b0, d0;
    int jrange1;
};

#define n2part_1 (*(struct n2part_1_ *) &n2part_)
#define n2part_2 (*(struct n2part_2_ *) &n2part_)

union u_bl3_ {
    struct s_m_1 {
        double rsi[401];
    } m_1;
    struct s_m_2 {
        double rsibb[401];
    } m_2;
} bl3_;

#define bl3_1 (bl3_.m_1)
#define bl3_2 (bl3_.m_2)

union u_bbbb_ {
    struct s_m_1 {
        int idelv, iv, ivp, idell, il, ilp;
    } m_1;
    struct s_m_2 {
        int ldelvi, ivi, ivip, ldelel, ll, llp;
    } m_2;
} bbbb_;

#define bbbb_1 (bbbb_.m_1)
#define bbbb_2 (bbbb_.m_2)

/* Initialized data */

struct s_energe_ {
    double e_1[246];
    int e_2[6];
    } energ_ = { {-54.99996, -54.86228, -54.58697, -54.17413, -53.62391, 
            -52.93648, -52.11211, -51.15108, -50.05374, -48.82049, -47.45179, 
            -45.94815, -44.31014, -42.53841, -40.63365, -38.59665, -36.42824, 
            -34.12937, -31.70105, -29.14439, -26.46061, -23.65103, -20.71709, 
            -17.66041, -14.48271, -11.18593, -7.77221, -4.24393, -.60374, 
            3.14531, 6.99978, 10.95566, 15.00818, 19.15136, 23.37787, 
            27.67681, 32.03237, 36.42278, 40.83668, 45.29436, 49.79246, 
            -31.89437, -31.77215, -31.52779, -31.16143, -30.67334, -30.06382, 
            -29.33328, -28.48222, -27.51123, -26.42099, -25.21229, -23.88603, 
            -22.44322, -20.88502, -19.21272, -17.42777, -15.53182, -13.52669, 
            -11.41446, -9.1975, -6.87848, -4.46049, -1.94714, .65736, 3.34788,
             6.11816, 8.95978, 11.8613, 14.80383, 17.75924, 20.71774, 
            23.71589, 0., 0., 0., 0., 0., 0., 0., 0., 0., -16.05019, -15.9464,
             -15.73896, -15.42815, -15.0144, -14.4983, -13.88057, -13.16213, 
            -12.34407, -11.42771, -10.41455, -9.30639, -8.10531, -6.81376, 
            -5.43459, -3.97121, -2.42768, -.80899, .87859, 2.62689, 4.42334, 
            6.24733, 8.06983, 9.90464, 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,
             0., 0., 0., 0., 0., 0., 0., -6.49343, -6.41131, -6.24732, 
            -6.00202, -5.67623, -5.27111, -4.78813, -4.22919, -3.59665, 
            -2.89345, -2.12325, -1.29074, -.40202, .5345, 1.50455, 2.48212, 
            3.46665, 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 
            0., 0., 0., 0., 0., 0., 0., 0., 0., 0., -1.76583, -1.70887, 
            -1.59552, -1.427, -1.20523, -.93302, -.61434, -.25504, .13641, 0.,
             0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 
            0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 
            -.17133, -.14341, 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 
            0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 
            0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.}, {41, 32, 24, 17, 9, 2} }
            ;

struct s_n2part_ {
    double fill_1[1];
    double e_2[4];
    int fill_3[1];
    } n2part_ = { {0}, {2., 1., 1.98957, 5.8e-6}, {0} };

struct s_like_ {
    int fill_1[1];
    char e_2[5];
    } like_ = { {0}, "N2N2" };


/* Table of constant values */

// FIXME static integer c__9 = 9;
// FIXME static integer c__1 = 1;
// FIXME static integer c__5 = 5;
static int cs__1 = 1;
static int cs__0 = 0;
static double c_b24 = 2.9723;
static double c_b25 = -.99569;
static double c_b26 = .09464;
static double c_b27 = 1.2962e-12;
static double c_b28 = -.13048;
static double c_b29 = -.03128;
static double c_b30 = 3.7969e-14;
static double c_b31 = 1.03681;
static double c_b32 = -.14336;
static int cs__2 = 2;
static int cs__3 = 3;
static double c_b43 = .180926;
static double c_b44 = -1.69153;
static double c_b45 = .18605;
static double c_b46 = .3;
static double c_b47 = 0.;
static double c_b49 = 6.6017e-16;
static double c_b50 = 2.59982;
static double c_b51 = -.31831;
static double c_b52 = 1.2481e-12;
static double c_b53 = -.57028;
static double c_b54 = .05983;
static double c_b55 = 5.2681e-13;
static double c_b56 = -.24719;
static double c_b57 = .00519;
static double c_b58 = 2.7518e15;
static double c_b59 = -25.38969;
static double c_b60 = 2.46542;
static int cs__4 = 4;
static int cs__5 = 5;
// FIXME static integer c__2 = 2;
static double c_b78 = .0825299;
static double c_b79 = -1.25562;
static double c_b80 = .12981;
static double c_b84 = 3.6611e-15;
static double c_b85 = 1.47688;
static double c_b86 = -.16537;
static double c_b87 = 6.1264e-10;
static double c_b88 = -2.25011;
static double c_b89 = .15289;
static double c_b90 = 7.982e-10;
static double c_b91 = -2.76152;
static double c_b92 = .21847;
static double c_b93 = 5.2868e-22;
static double c_b94 = 7.66253;
static double c_b95 = -.77527;
static double c_b112 = 119.261;
static double c_b113 = -3.78587;
static double c_b114 = .34024;
static double c_b115 = 9.3777e-12;
static double c_b116 = -.66548;
static double c_b117 = .0033;
static double c_b118 = 3.0395e-13;
static double c_b119 = .24728;
static double c_b120 = -.06607;
static double c_b183 = 1e-6;
static double c_b186 = 1.5;

#define temp (blockin_1.temp)
#define fnumin (blockin_1.fnumin)
#define fnumax (blockin_1.fnumax)
#define dnu (blockin_1.dnu)
#define slit (app3a_1.slit)
#define dx (app3a_1.dx)
#define rsilo (rsilo_1.rsilo)
#define omeg (bba_1.omeg)
#define rsi (bba_1.rsi)
#define rsigg (bba_1.rsigg)
#define nsol (bbc_1.nsol)
#define like (like_1.like)
#define ik1k0 (k1k0_1.ik1k0)
#define ibound (bbb_1.ibound)

/* TKS ****** SUBROUTINE N2N2TKS(T, F) ***************************************/
Numeric n2n2tks_(double t, double f)
{
    /* System generated locals */
    int s__1;
    double ret_val;

    /* Local variables */
    double hexa[10], quad[10], freq[10], e;
    int i__;
    double s, x, t1, t2, t3, t4;
    int ij, nf, jj;
    double rslow1, si;
    int nr;
    double ss[1], tt[2];
    extern /* Subroutine */ int bound32_(double *, double *, int 
            *), bound54_(double *, double *, int *);
    double tksabs[5];
    extern /* Subroutine */ int spline_(int *, int *, int *, 
            double *, double *, double *, double *, 
            double *, double *, int *, double *);
    double dtrans[10], abscoef[10];
    extern /* Subroutine */ int addspec_(double *, double *, 
            double *, double *, double *, double *, 
            double *, int *, double *, double *, int *, 
            int *, int *, int *, int *, int *);
    double eps, alfatot[10];
    extern /* Subroutine */ int partsum_(double *);

/*     ========================================= */
/*     Copyright (C) Aleksandra Borysow, 1987) */
/*     ==================================================================== */
/*     PROGRAM PREPARED BY ALEKSANDRA BORYSOW (APRIL'1987) */
/*     (UNIVERSITY OF TEXAS AT AUSTIN, PHYSICS DEPARTMENT) */
/*     ORIGINAL VERSION: WRITTEN ON CYBER */

/*     PROGRAM GENERATES N2-N2 COLLISION-INDUCED SPECTRA AT */
/*     TEMPERATURES BETWEEN 50 TO 300 K. */
/*     CIA SPECTRA MODELED AFTER PAPER (*) */
/*     ALEKSANDRA BORYSOW AND LOTHAR FROMMHOLD, */
/*     ASTROPHYSICAL JOURNAL, VOL. 311, PAGES 1043-1057, (1986) */

/*     REVISED BY GLENN ORTON (1989) - TO WORK ON SUN WORKSTATIONS */
/*     AND ON THE VAX MACHINES (FORTRAN-77) */
/*     PASSES STANDARD TEST ON SUN, AT 200K (JULY 1992) */
/*     ==================================================================== */

/*     ALSO IN REVISION: DOUBLE PRECISION FOR ALL F.P. VARIABLES */

/*     ==================================================================== */

/*     HISTORY: */

/*     2001-02-28 THOMAS KUHN: */
/*     CHANGE OF LINES */
/*       RSILO(I)=DLOG(RSI(I)*1.E80) */
/*     TO */
/*       RSILO(I)=(DLOG(RSI(I))+80.0D0*DLOG(10.0D0)) */
/*     BECAUSE OF OVERFLOW PROBLEMS. */
/*     COSMETICS FOR THE CODE TO BE FASTER READABLE. */
/*     CHANGE OF OUTPUT FILE NAME. */
/*     CHANGE OF OUTPUT FILE CONTENT */

/*     ==================================================================== */

/* TKS*      IMPLICIT REAL*8 (A-H,O-Z) */

/* TKS  INPUT/OUTPUT VARIABLES */
/*      REAL T, F */

    ret_val = 0.;

/*     TEMP   = TEMPERATURE IN KELVIN, SHOULD BE BETWEEN 50. AND 300. */
/*     FNUMIN = LOWEST FREQUENCY IN CM-1, FOR LISTING OF ALPHA(FNU) */
/*     FNUMAX = HIGHEST FREQUENCY IN CM-1, FOR LISTING OF ALPHA(FNU) */
/*     LINE SHAPE MODELLING WILL BE MOST ACCURATE WITHIN RANGE OF */
/*     R-T SPECTRAL INTENSITIES AS 1:100. */
/*     DNU    = FREQUENCY INCREMENT IN CM-1. DNU SHOULD BE CHOSEN SO */
/*              THAT NOT MORE THAN 10 STEPS ARE NEEDED TO GO FROM */
/*              FNUMIN TO FNUMAX (ELSE ARRAY DIMENSIONS OF FREQ,ABSCOEF */
/*              MUST BE ADJUSTED IN ADDEM). */


/*              USER: */
/*       ----- */
/*      EDIT ONLY HERE: TEMP (K), MIN. FREQ. (CM^-1)= FNUMIN, */
/*      MAX. FREQ. =  FNUMAX, STEP = DNU, SLITWIDTH (CM^-1)=SLIT */
/*      (SLIT=4.3 IS EQUIVALENT TO THAT OF VOYAGER SPECTRA, ONLY BOUND BOUND */
/*      SPECTRA ARE CONVOLUTED WITH THIS SLITWIDTH, THE FREE FREE SPECTRA */
/*      ARE FAR TOO BROAD FOR THE SLITWIDTH FUNCTION TO MATTER, */
/*      LEAVE LIKE = 1 (FOR LIKE PAIRS,  AS N2-N2) */
/*      THE PROGRAM WILL ASSUME EQUILIBRIUM N2, */
/*      ALLOWED TEMPERATURE RANGE: 50-300K (DO NOT  EXTEND IT BEYOND THESE LIMITS!) */
/*      IF QUESTIONS: CONTACT ABORYSOW@NBI.DK */
/* TKS*      NF=INT((FNUMAX-FNUMIN)/DNU+0.5)+1 */
/* TKS*      IF (NF.GT.10) NF=10 */
/* TKS*      FNUMAX=FNUMIN+FLOAT(NF-1)*DNU */

/* TKS  INPUT TEMPERATURE (K) CHECK OF RANGE */
    if (t < 50. || t > 300.) {
      ostringstream os;
      os  << "out of T range ( 50<T<300)! return without calc.!" <<"\n";
      throw runtime_error(os.str());
      goto L999;
    }
    temp = t;

/*     *********************** INPUT DATA FROM USER *********************** */
/*     FNUMIN = MINIMUM FREQENCY [CM^-1] */
    fnumin = f / 29979245800.;
/*     FNUMAX = MAXIMUM FREQENCY [CM^-1] */
    fnumax = fnumin;
/*     ONLY ONE FREQUENCY PER CALL */
    nf = 1;
/*     DEFAULT VALUE OF FREQUENCY STEP [CM^-1] */
    dnu = 10.;
/*     DEFAULT VALUE */
    like = 1;
/*     SLIT = SLITWIDTH [CM^-1] */
/*     SLIT=4.3 IS EQUIVALENT TO THAT OF VOYAGER SPECTRA, ONLY BOUND BOUND */
/*     SPECTRA ARE CONVOLUTED WITH THIS SLITWIDTH, THE FREE FREE SPECTRA */
/*     ARE FAR TOO BROAD FOR THE SLITWIDTH FUNCTION TO MATTER. */
    slit = 4.3;
/*     ******************************************************************** */

/* TKS*      WRITE (6,14) LGAS,TEMP,FNUMIN,FNUMAX,DNU,NF-1 */
/* TKS*14    FORMAT(' ABSORPTION SPECTRA OF ',A5,' AT',F8.1,' K'/ */
/* TKS*     $   1X,43(1H=),/ */
/* TKS*     1' MIN.FREQ.=',F8.1,' CM-1',10X,'MAX.FREQ.=',F8.1,' CM-1',10X, */
/* TKS*     2'FREQ.INCREMENT=',F8.2,' CM-1',5X,'IN',I5,' STEPS'//) */


    partsum_(&temp);


/*     THE N2-N2 SPECTRA   FOR 50-300K */
/*     ================================ */

    x = log(temp);
    s__1 = nf;
    for (i__ = 1; i__ <= s__1; ++i__) {
/*         FREQ(I)=FNUMIN+FLOAT(I-1)*DNU */
        freq[i__ - 1] = fnumin;
        alfatot[i__ - 1] = 0.;
/* L10: */
        abscoef[i__ - 1] = 0.;
    }


/*    ==================================================================== */


    jj = 1;
L442:
/* L1023: */
    ++jj;
    if (jj == 42) {
        goto L444;
    }
    goto L442;
/*     EB(JJ,IV) JJ-ROTATIONAL LEVEL "L", IV- VIBRATIONAL LEVEL "V"; */
L444:



/*     ==================================================================== */

/*     QUADRUPOLAR INDUCTION: (50-300K) LAMBDA1,LAMBDA2,LAMBDA,L=2023&0223 */
/*     ------------------------------------------------------------------- */

    eps = 1e-5;
    tt[0] = 10.;
    bound32_(&temp, rsi, &nsol);
    ij = 0;
    rslow1 = 0.;
    s__1 = nsol;
    for (i__ = 1; i__ <= s__1; ++i__) {
        ++ij;
/*        MOD CAN BE ONLY 0 OR 1 OR 2 */
        if (ij % 3 == 0) {
            rslow1 = 1.5e-60;
        }
        if (ij % 3 == 1) {
            rslow1 = 1.7e-60;
        }
        if (ij % 3 == 2) {
            rslow1 = 1.6e-60;
        }
        if (rsi[i__ - 1] < 1e-60) {
            rsi[i__ - 1] = rslow1;
        }
/* TKS*      RSILO(I)=DLOG(RSI(I)*1.D80) */
        rsilo[i__ - 1] = log(rsi[i__ - 1]) + log(10.) * 80.;
        omeg[i__ - 1] = (double) (i__ - 1) * dx;
/* L88: */
    }

/* L9991: */

    spline_(&nsol, &cs__1, &cs__0, &eps, omeg, rsilo, tt, ss, &si, &nr, rsigg)
            ;

    ik1k0 = 1;
    ibound = 1;
/*       B-C LINESHAPE HERE */
/*       THESE VALUES (S,T1,T2) REPLACE VALUES GIVEN IN PAPER (*): */
/*       PUBLISHED IN AN ERRATUM, ASTROPHYSICAL JOURNAL, VOL.320, P.437 */
/*       (1987) */
    s = c_b24 * exp((c_b26 * x + c_b25) * x);
    t1 = c_b27 * exp((c_b29 * x + c_b28) * x);
    t2 = c_b30 * exp((c_b32 * x + c_b31) * x);
    e = 0.;
    t3 = 0.;
    t4 = 0.;

    addspec_(&s, &e, &t1, &t2, &t3, &t4, &temp, &nf, freq, abscoef, &cs__0, &
            like, &cs__2, &cs__0, &cs__2, &cs__3);
    s__1 = nf;
    for (i__ = 1; i__ <= s__1; ++i__) {
        quad[i__ - 1] = abscoef[i__ - 1];
/* L20: */
        alfatot[i__ - 1] = abscoef[i__ - 1] + alfatot[i__ - 1];
    }



/*     ==================================================================== */

/*     HEXADECAPOLE COMPONENTS: LAMBDA1,LAMBDA2,LAMBDA,L=4045&0445 */
/*     ----------------------------------------------------------- */

    bound54_(&temp, rsi, &nsol);
    ij = 0;
    s__1 = nsol;
    for (i__ = 1; i__ <= s__1; ++i__) {
        ++ij;
/*     MOD CAN BE ONLY 0 OR 1 OR 2 */
        if (ij % 3 == 0) {
            rslow1 = 1.5e-60;
        }
        if (ij % 3 == 1) {
            rslow1 = 1.7e-60;
        }
        if (ij % 3 == 2) {
            rslow1 = 1.6e-60;
        }
        if (rsi[i__ - 1] < 1e-60) {
            rsi[i__ - 1] = rslow1;
        }
/* TKS         RSILO(I)=DLOG(RSI(I)*1.E80) */
        rsilo[i__ - 1] = log(rsi[i__ - 1]) + log(10.) * 80.;
/* L111: */
        omeg[i__ - 1] = (double) (i__ - 1) * dx;
    }
    spline_(&nsol, &cs__1, &cs__0, &eps, omeg, rsilo, tt, ss, &si, &nr, rsigg)
            ;

/*     --------------------------- */
/*       TEMPERATURES 50-140K */
/*     --------------------------- */

    if (temp >= 140.) {
        goto L333;
    }

    s = c_b43 * exp((c_b45 * x + c_b44) * x);
    e = c_b46 * exp((c_b47 * x + c_b47) * x);
    t1 = c_b49 * exp((c_b51 * x + c_b50) * x);
    t2 = c_b52 * exp((c_b54 * x + c_b53) * x);
    t3 = c_b55 * exp((c_b57 * x + c_b56) * x);
    t4 = c_b58 * exp((c_b60 * x + c_b59) * x);

    ik1k0 = 0;
    ibound = 1;
    addspec_(&s, &e, &t1, &t2, &t3, &t4, &temp, &nf, freq, abscoef, &cs__0, &
            like, &cs__4, &cs__0, &cs__4, &cs__5);
    s__1 = nf;
    for (i__ = 1; i__ <= s__1; ++i__) {
        hexa[i__ - 1] = abscoef[i__ - 1];
        /*
          s_wsle(&io___25);
          do_lio(&c__9, &c__1, " T=50-140K: HEXA(", (ftnlen)17);
          do_lio(&c__2, &c__1, (char *)&i__, (ftnlen)sizeof(int));
          do_lio(&c__9, &c__1, ") =", (ftnlen)3);
          do_lio(&c__5, &c__1, (char *)&abscoef[i__ - 1], (ftnlen)sizeof(
          double));
          e_wsle();
        */
/* L50: */
        alfatot[i__ - 1] += abscoef[i__ - 1];
    }
    goto L334;

/*     --------------------------- */
/*       TEMPERATURES 140-300K */
/*     --------------------------- */

L333:
    ik1k0 = 0;
    ibound = 1;
    s = c_b78 * exp((c_b80 * x + c_b79) * x);
    e = c_b46 * exp((c_b47 * x + c_b47) * x);
    t1 = c_b84 * exp((c_b86 * x + c_b85) * x);
    t2 = c_b87 * exp((c_b89 * x + c_b88) * x);
    t3 = c_b90 * exp((c_b92 * x + c_b91) * x);
    t4 = c_b93 * exp((c_b95 * x + c_b94) * x);

    addspec_(&s, &e, &t1, &t2, &t3, &t4, &temp, &nf, freq, abscoef, &cs__0, &
            like, &cs__4, &cs__0, &cs__4, &cs__5);
    s__1 = nf;
    for (i__ = 1; i__ <= s__1; ++i__) {
        hexa[i__ - 1] = abscoef[i__ - 1];
        /*
          s_wsle(&io___26);
          do_lio(&c__9, &c__1, " T=140-300K: HEXA(", (ftnlen)18);
          do_lio(&c__2, &c__1, (char *)&i__, (ftnlen)sizeof(int));
          do_lio(&c__9, &c__1, ") =", (ftnlen)3);
          do_lio(&c__5, &c__1, (char *)&abscoef[i__ - 1], (ftnlen)sizeof(
          double));
          e_wsle();
        */
/* L550: */
        alfatot[i__ - 1] += abscoef[i__ - 1];
    }

/*     ==================================================================== */

/*     DOUBLE TRANSITIONS: LAMBDA1,LAMBDA2,LAMBDA,L=2,2,3,3 */
/*     ---------------------------------------------------- */

/*     --------------------------- */
/*       TEMPERATURES 50-300K */
/*     --------------------------- */

L334:
    ik1k0 = 1;
    ibound = 0;
/* X        S=Y(X,1.19261D-58, -3.78587,0.34024) */
    s = c_b112 * exp((c_b114 * x + c_b113) * x);
    t1 = c_b115 * exp((c_b117 * x + c_b116) * x);
    t2 = c_b118 * exp((c_b120 * x + c_b119) * x);
    t3 = 0.;
    t4 = 0.;
    addspec_(&s, &e, &t1, &t2, &t3, &t4, &temp, &nf, freq, abscoef, &cs__0, &
            like, &cs__2, &cs__2, &cs__3, &cs__3);
    s__1 = nf;
    for (i__ = 1; i__ <= s__1; ++i__) {
        dtrans[i__ - 1] = abscoef[i__ - 1];
/* L650: */
        alfatot[i__ - 1] += abscoef[i__ - 1];
    }

/*     ==================================================================== */

/*     ANISOTROPIC OVERLAP NEGLECTED (LAMBDA1,LAMBDA2,LAMBDA,L=0212) */
/*     SINCE THIS TERM IS EXTREMELY SMALL */

/*     ==================================================================== */

/* TKS*      PRINT 154, FREQ(1),FREQ(NF),FREQ(2)-FREQ(1),TEMP */
/* TKS*      PRINT 156, (ALFATOT(I),I=1,NF) */
/* TKS*154   FORMAT(///' ABSORPTION COEFFICIENT ALPHA(FNU), FROM ',F5.1, */
/* TKS*     $' CM-1 TO',F7.1,' CM-1, AT',F6.2,' CM-1 INCREMENTS, AT T=', */
/* TKS*     $F7.2,' K, IN UNITS OF CM-1 AMAGAT-2'/) */
/* TKS*156   FORMAT(' ',10D13.5) */
/* TKS* OPEN(UNIT=10, FILE='OUT', STATUS='UNKNOWN') */
/* TKS* WRITE(10, 2929) (FREQ(I), ALFATOT(I), I=1, NF) */
/* TKS*C        WRITE(10, 2929) (FREQ(I), QUAD(I), HEXA(I) ALFATOT(I), I=1, NF) */
/* TKS*2929     FORMAT(F10.3, E12.4) */

/* TKS*      STOP */



/* TKS FILL OUTPUT VARIABLE */
    tksabs[0] = quad[0];
    tksabs[1] = hexa[0];
    tksabs[2] = dtrans[0];
    tksabs[3] = alfatot[0];
    ret_val = alfatot[0];
/* TKS      print*,'QUAD(1),HEXA(1),DTRANS(1)=',QUAD(1),HEXA(1),DTRANS(1) */
L999:
    return ret_val;
} /* n2n2tks_ */

#undef temp
#undef fnumin
#undef fnumax
#undef dnu
#undef slit
#undef dx
#undef rsilo
#undef omeg
#undef rsi
#undef rsigg
#undef nsol
#undef like
#undef ik1k0
#undef ibound

#define wnrmax3 (app3a_1.wnrmax3)
#define rsilo (rsilo_1.rsilo)
#define omeg (bba_2.omeg)
#define rsigg (bba_2.rsigg)
#define beta (bba_2.beta)
#define nsol (bbc_1.nsol)
#define ibound (bbb_1.ibound)
#define q1 (n2part_1.q1)
#define wn2 (n2part_1.wn2)
#define b01 (n2part_1.b01)
#define d01 (n2part_1.d01)
#define jrange2 (n2part_1.jrange2)



/* ########################################################################## */


/* Subroutine */ int addspec_(double *g0, double *ep, double *
        tau1, double *tau2, double *tau5, double *tau6, 
        double *temp, int *nf, double *freq, double *abscoef,
         int * /* mp */, int *like, int *lambda1, int *lambda2, 
        int *lambda, int * /* lvalue */)
{
    /* Initialized data */

    static double closchm = 2.68675484e19;
    static double boltzwn = .6950304;
    static double hbar = 1.054588757e-27;
    static double pi = 3.1415926535898;
    static double clight = 2.997925e10;

    /* Format strings */
    /*
    static char fmt_20[] = "(/\002 LAMBDA1,LAMBDA2, LAMBDA,LVALUE=\002,2i3,2"
            "x,2i3,\002 COMPONENT.\002/15x,\002LINE SHAPE PARAMETERS:\002,6d1"
            "2.3,5x,\002G(0)=\002,d12.3/)";
    */

    /* System generated locals */
    int s__1, s__2, s__3, s__4, s__5, s__6;
    double d__1, d__2;

    /* Builtin functions */
    /*
    integer s_wsfe(cilist *), do_fio(integer *, char *, ftnlen), e_wsfe(void),
             s_wsle(cilist *), do_lio(integer *, integer *, char *, ftnlen), 
            e_wsle(void);
    */

    /* Local variables */
    int list, jsum;
    extern double bgama_(double *, double *, double *, 
            double *, double *, double *, double *);
    int i__, j;
    double calib, p;
    int i1, j1, i2, j2;
    double p1, p2, omega1, omega2;
    int ip, jp, iq;
    double twopic;
    int jplusl, ip1, jp1, ip2, jp2;
    double fac, cgs, xbg, wkf, frq, wki;
    extern double specfct_(double *, double *, double *, 
            double *, int *, double *), clebsqr_(int *, 
            int *, int *);
    double cg1s, cg2s;

    /* Fortran I/O blocks */
    /*
    static cilist io___38 = { 0, 6, 0, fmt_20, 0 };
    static cilist io___40 = { 0, 6, 0, 0, 0 };
    */


/*     THIS PROGRAM GENERATES LISTING OF R-T CIA  ALFA(OMEGA) */
/*     IF EITHER LAMBDA1 OR LAMBDA2 EQUAL TO ZERO - SINGLE TRANSITIONS; */
/*     DOUBLE TRANSITIONS ARE ASSUMED OTHERWISE. */
/*     LIKE=1 FOR LIKE SYSTEMS (AS H2-H2), SET LIKE=0 ELSE. */

/*     COMMON/BB/OMEG(201),RSI(201),RSIGG(201),NSOL,BETA */
/*     COMMON/APP3/SLIT,DX,NSRI,WNRMAX3,NS,NSRIUP */
/*     DIMENSION ABSCOEF(NF),FREQ(NF) */
    /* Parameter adjustments */
    --abscoef;
    --freq;

    /* Function Body */

    twopic = 2. * pi * clight;
    if (*like != 1) {
        *like = 0;
    }
/*        TAKE CARE OF FACTOR OF 1.E-60 HERE. */
/* Computing 2nd power */
    d__1 = pi;
/* Computing 2nd power */
    d__2 = closchm * 1e-30;
    calib = twopic * (d__1 * d__1 * 4. / (hbar * 3. * clight)) * (d__2 * d__2)
            ;
    calib /= (double) (*like + 1);
    beta = 1. / (boltzwn * *temp);
    list = *nf;
    s__1 = list;
    for (i__ = 1; i__ <= s__1; ++i__) {
/* L88: */
        abscoef[i__] = 0.;
    }

/*     ROTATIONAL SPECTRUM FOR THE DETAILED LISTING   ******************* */
    /*
      s_wsfe(&io___38);
      do_fio(&c__1, (char *)&(*lambda1), (ftnlen)sizeof(int));
      do_fio(&c__1, (char *)&(*lambda2), (ftnlen)sizeof(int));
      do_fio(&c__1, (char *)&(*lambda), (ftnlen)sizeof(int));
      do_fio(&c__1, (char *)&(*lvalue), (ftnlen)sizeof(int));
      do_fio(&c__1, (char *)&(*g0), (ftnlen)sizeof(double));
      do_fio(&c__1, (char *)&(*ep), (ftnlen)sizeof(double));
      do_fio(&c__1, (char *)&(*tau1), (ftnlen)sizeof(double));
      do_fio(&c__1, (char *)&(*tau2), (ftnlen)sizeof(double));
      do_fio(&c__1, (char *)&(*tau5), (ftnlen)sizeof(double));
      do_fio(&c__1, (char *)&(*tau6), (ftnlen)sizeof(double));
      d__1 = *g0 * bgama_(&c_b47, tau1, tau2, ep, tau5, tau6, temp);
      do_fio(&c__1, (char *)&d__1, (ftnlen)sizeof(double));
      e_wsfe();
    */
    if (*lambda1 == 0 || *lambda2 == 0) {
        goto L152;
    }
    jplusl = jrange2 + max(*lambda1,*lambda2);

    /*
      s_wsle(&io___40);
      do_lio(&c__9, &c__1, "LAMBDA1,LAMBDA2,ABSCOEF(1)=", (ftnlen)27);
      do_lio(&c__2, &c__1, (char *)&(*lambda1), (ftnlen)sizeof(int));
      do_lio(&c__2, &c__1, (char *)&(*lambda2), (ftnlen)sizeof(int));
      do_lio(&c__5, &c__1, (char *)&abscoef[1], (ftnlen)sizeof(double));
      e_wsle();
    */
    jsum = 0;
    s__1 = jrange2;
    for (i1 = 1; i1 <= s__1; ++i1) {
        j1 = i1 - 1;
        s__2 = jplusl;
        for (ip1 = 1; ip1 <= s__2; ++ip1) {
            jp1 = ip1 - 1;
            cg1s = clebsqr_(&j1, lambda1, &jp1);
            if (cg1s <= 0.) {
                goto L150;
            } else {
                goto L130;
            }
L130:
            s__3 = j1 * (j1 + 1);
            p1 = (double) (2 * j1 + 1) * wn2[1 + j1 % 2 - 1] * exp(
                    -1.4387859 / *temp * ((b01 - (double) s__3 * d01) * (
                    double) s__3)) / q1;
            ++jsum;
            s__3 = jp1 * ip1;
            s__4 = j1 * i1;
            omega1 = (b01 - (double) s__3 * d01) * (double) s__3 - (
                    b01 - (double) s__4 * d01) * (double) s__4;
            s__3 = jrange2;
            for (i2 = 1; i2 <= s__3; ++i2) {
                j2 = i2 - 1;
                s__4 = jplusl;
                for (ip2 = 1; ip2 <= s__4; ++ip2) {
                    jp2 = ip2 - 1;
                    cg2s = clebsqr_(&j2, lambda2, &jp2);
                    if (cg2s <= 0.) {
                        goto L148;
                    } else {
                        goto L132;
                    }
L132:
                    s__5 = j2 * (j2 + 1);
                    p2 = (double) (2 * j2 + 1) * wn2[1 + j2 % 2 - 1] * 
                            exp(-1.4387859 / *temp * ((b01 - (double) 
                            s__5 * d01) * (double) s__5)) / q1;
                    s__5 = jp2 * ip2;
                    s__6 = j2 * i2;
                    omega2 = (b01 - (double) s__5 * d01) * (double) 
                            s__5 - (b01 - (double) s__6 * d01) * (
                            double) s__6;
                    fac = calib * p1 * p2 * cg1s * cg2s;
                    s__5 = list;
                    for (i__ = 1; i__ <= s__5; ++i__) {
                        frq = freq[i__] - omega1 - omega2;
                        wki = freq[i__] * (1. - exp(-beta * freq[i__]));
                        wkf = wki * fac;
                        xbg = *g0 * bgama_(&frq, tau1, tau2, ep, tau5, tau6, 
                                temp);
                        if (ibound == 0) {
                            goto L555;
                        }
                        if (abs(frq) <= wnrmax3) {
                            xbg += specfct_(&frq, omeg, rsilo, rsigg, &nsol, &
                                    beta);
                        }
L555:
                        abscoef[i__] += xbg * wkf;
/* L146: */
                    }
L148:
                    ;
                }
            }
L150:
            ;
        }
    }
    goto L2222;
/*     SINGLE TRANSITIONS AT NITROGEN'S ROTATIONAL FREQUENCIES */
/*     ======================================================= */
L152:
    jplusl = jrange2 + *lambda;
    s__2 = jrange2;
    for (i__ = 1; i__ <= s__2; ++i__) {
        j = i__ - 1;
        s__1 = jplusl;
        for (ip = 1; ip <= s__1; ++ip) {
            jp = ip - 1;
            cgs = clebsqr_(&j, lambda, &jp);
            if (cgs <= 0.) {
                goto L200;
            } else {
                goto L210;
            }
L210:
            s__4 = j * (j + 1);
            p = (double) (2 * j + 1) * wn2[1 + j % 2 - 1] * exp(
                    -1.4387859 / *temp * ((b01 - (double) s__4 * d01) * (
                    double) s__4)) / q1;
            ++jsum;
            s__4 = jp * ip;
            s__3 = j * i__;
            omega1 = (b01 - (double) s__4 * d01) * (double) s__4 - (
                    b01 - (double) s__3 * d01) * (double) s__3;
            fac = calib * p * cgs;
            s__4 = list;
            for (iq = 1; iq <= s__4; ++iq) {
                frq = freq[iq] - omega1;
/*               XWKI=FREQ(IQ)*(1.-EXP(-BETA*FREQ(IQ))) */
                wki = freq[iq] * (1. - exp(-beta * freq[iq]));
                wkf = wki * fac;
                xbg = *g0 * bgama_(&frq, tau1, tau2, ep, tau5, tau6, temp);
                if (ibound == 0) {
                    goto L444;
                }
                if (abs(frq) <= wnrmax3) {
                    xbg += specfct_(&frq, omeg, rsilo, rsigg, &nsol, &beta);
                }
L444:
                abscoef[iq] += xbg * wkf;
/* L199: */
            }
L200:
            ;
        }
    }

L2222:
/* TKS 2222   PRINT 44,(ABSCOEF(I),I=1,LIST) */
/* L44: */
    return 0;
} /* addspec_ */

#undef wnrmax3
#undef rsilo
#undef omeg
#undef rsigg
#undef beta
#undef nsol
#undef ibound
#undef q1
#undef wn2
#undef b01
#undef d01
#undef jrange2

#define q (n2part_2.q)
#define wn2 (n2part_2.wn2)
#define b0 (n2part_2.b0)
#define d0 (n2part_2.d0)
#define jrange1 (n2part_2.jrange1)

/* Subroutine */ int partsum_(double *temp)
{
    /* System generated locals */
    int s__1;

    /* Local variables */
    int j;
    double dq;

/*     N2 ROTATIONAL PARTITION SUM Q = Q(T). */



/*     Q,B0,D0,WN2 - PARTITION FCT., ROT.CONSTANTS, WEIGHTS FOR N2 */
    q = 0.;
    j = 0;
L50:
    s__1 = j * (j + 1);
    dq = (double) (2 * j + 1) * wn2[1 + j % 2 - 1] * exp(-1.4387859 * ((
            b0 - (double) s__1 * d0) * (double) s__1) / *temp);
    q += dq;
    ++j;
    if (dq > q / 900.) {
        goto L50;
    }
    jrange1 = j;
/* TKS      PRINT 30, Q, JRANGE1 */

/* L30: */
    return 0;
} /* partsum_ */

#undef q
#undef wn2
#undef b0
#undef d0
#undef jrange1

#define slit (app3a_1.slit)
#define dx (app3a_1.dx)
#define wnrmax3 (app3a_1.wnrmax3)
#define nsri (app3b_1.nsri)
#define ns (app3b_1.ns)
#define nsriup (app3b_1.nsriup)
#define rsi (bl3_1.rsi)

/* Subroutine */ int profile_(double *x, double *y)
{
    /* System generated locals */
    int s__1;

    /* Local variables */
    int i__;
    double slope;
    int n1;
    double x0;
    int nc;
    double dr;
    int no;
    double xi;
    int nu;

/*     A TRIANGULAR SLIT FUNCTION IS USED. */


/*     COMMON/APP3/SLIT,DX,NSRI,WNRMAX3,NS,NSRIUP */

    if (*y < 0.) {
        goto L105;
    } else if (*y == 0) {
        goto L106;
    } else {
        goto L1;
    }
L1:
    x0 = nsri + 1. + *x / dx;
    nc = (int) x0;
    n1 = nc + 1;
    slope = *y / slit;
    nu = (int) (x0 - ns);
    if (nu < 1) {
        nu = 1;
    }
    if (nu > nsriup) {
        return 0;
    }
    no = (int) (x0 + ns);
    if (no > nsriup) {
        no = nsriup;
    }
    if (no < 1) {
        return 0;
    }
    if (nc > nsriup) {
        nc = nsriup;
    }
    if (nc <= 1) {
        goto L101;
    }
    s__1 = nc;
    for (i__ = nu; i__ <= s__1; ++i__) {
        xi = (i__ - 1.) * dx - wnrmax3;
        dr = slope * (xi - (*x - slit));
        if (dr <= 0.) {
            goto L100;
        }
        rsi[i__ - 1] += dr;
L100:
        ;
    }
L101:

    if (nc >= nsriup) {
        return 0;
    }
    if (n1 < 1) {
        n1 = 1;
    }
    s__1 = no;
    for (i__ = n1; i__ <= s__1; ++i__) {
        xi = (i__ - 1.) * dx - wnrmax3;
        dr = *y - slope * (xi - *x);
        if (dr <= 0.) {
            goto L102;
        }
        rsi[i__ - 1] += dr;
L102:
        ;
    }
    return 0;
L105:
/* TKS  105 PRINT 10,SLIT */
/* TKS   10 FORMAT(/' A TRIANGULAR SLIT FUNCTION OF',F6.3,' CM-1 HALFWIDTH IS */
/* TKS     ' USED'/) */
L106:
    return 0;
} /* profile_ */

#undef slit
#undef dx
#undef wnrmax3
#undef nsri
#undef ns
#undef nsriup
#undef rsi


/* X    FUNCTION SPECFCT(FREQ,OMEGA,PHI,PHI2,N,RTEMP) */

double specfct_(double *freq, double *omega, double *phi, 
        double *phi2, int *n, double *rtemp)
{
    /* System generated locals */
    double ret_val;

    /* Local variables */
    double tfac, f, gp, si;
    int nr;
    extern /* Subroutine */ int ixpolat_(int *, int *, int *, 
            double *, double *, double *, double *, 
            double *, double *, int *, double *);


/*     THIS INTERPOLATES THE SPECTRAL FUNCTION PHI(FREQ) DEFINED AT */
/*     OMEGA(N) AS PHI(N). PHI2 IS THE SECOND DERIVATIVE AT OMEGA */
/*     WHICH MUST BE OBTAINED FIRST (USE SPLINE FOR THAT PURPOSE). */
/*     RTEMP IS THE RECIPROCAL TEMPERATURE IN CM-1 UNITS. */
/*     NOTE THAT WE INTERPOLATE 1.E80 TIMES THE LOGARITHM OF PHI(OMEGA) */
/*     NOTE THAT IN GSO'S REVISION, THIS FACTOR IS REMOVED. */
/*     (REVISION MODIFIED) */



/*      PRINT*,'FREQ =',FREQ */
/*      PRINT*,'OMEGA=',OMEGA */
/*      PRINT*,'RTEMP=',RTEMP */
/*      PRINT*,'PHI  =',PHI */
/*      PRINT*,'PHI2 =',PHI2 */
    /* Parameter adjustments */
    --phi2;
    --phi;
    --omega;

    /* Function Body */
    tfac = 0.;
    f = *freq;
    if (f >= 0.) {
        goto L20;
    } else {
        goto L10;
    }
L10:
    f = abs(f);
    tfac = -(*rtemp) * f;
L20:
    if (f <= omega[*n]) {
        goto L30;
    }
    ret_val = exp(-(phi[*n - 1] - phi[*n]) * (f - omega[*n]) / (omega[*n] - 
            omega[*n - 1]) + phi[*n] + tfac) * 1e-80;
/*      print*,' (A) SPECFCT=',SPECFCT */
/* X    SPECFCT=DEXP(-(PHI(N-1)-PHI(N))*(F-OMEGA(N))/ */
/* X   $(OMEGA(N)-OMEGA(N-1))+PHI(N)+TFAC) */
    return ret_val;
/* 30   PRINT*,'SI,NR,PHI2=', */
/*     &        SI,NR,PHI2 */
/*      CALL IXPOLAT(N,1,0,1.D-6,OMEGA,PHI,F,GP,SI,NR,PHI2) */
L30:
    ixpolat_(n, &cs__1, &cs__0, &c_b183, &omega[1], &phi[1], &f, &gp, &si, &
            nr, &phi2[1]);
    ret_val = exp(tfac + gp) * 1e-80;
/* X    SPECFCT=DEXP(TFAC+GP) */
/*      print*,' (B) GP,SPECFCT=',GP,SPECFCT */

    return ret_val;
} /* specfct_ */
#define slit (app3a_1.slit)
#define dx (app3a_1.dx)
#define wnrmax3 (app3a_1.wnrmax3)
#define nsri (app3b_1.nsri)
#define ns (app3b_1.ns)
#define nsriup (app3b_1.nsriup)
#define eb (energ_1.eb)
#define niv (energ_1.niv)
#define nlines (dimer_1.nlines)
#define rsibb (bl3_2.rsibb)
#define ldelvi (bbbb_2.ldelvi)
#define ivi (bbbb_2.ivi)
#define ivip (bbbb_2.ivip)
#define ldelel (bbbb_2.ldelel)
#define ll (bbbb_2.ll)
#define llp (bbbb_2.llp)

/* Subroutine */ int bound32_(double *temp, double *rsi, int *
        nsol)
{
    /* Initialized data */

    static int ldelvis[63] = { 0,0,0,0,0,0,0,0,0,0,1,1,1,1,1,1,1,1,1,1,1,
            1,1,1,1,1,2,2,2,2,2,2,2,2,2,2,2,2,2,2,2,2,3,3,3,3,3,3,3,3,3,3,3,3,
            3,4,4,4,4,4,4,4,4 };
    static int ivis[63] = { 0,0,1,1,2,2,3,3,4,4,0,0,0,0,1,1,1,1,2,2,2,2,
            3,3,3,3,0,0,0,0,1,1,1,1,2,2,2,2,3,3,3,3,0,1,2,0,1,2,0,1,0,1,0,1,2,
            0,1,0,1,0,1,0,1 };
    static int ivips[63] = { 0,0,1,1,2,2,3,3,4,4,1,1,1,1,2,2,2,2,3,3,3,3,
            4,4,4,4,2,2,2,2,3,3,3,3,4,4,4,4,5,5,5,5,3,4,5,3,4,5,3,4,3,4,3,4,5,
            4,5,4,5,4,5,4,5 };
    static int ldelels[63] = { 1,3,1,3,1,3,1,3,1,3,-3,-1,1,3,-3,-1,1,3,
            -3,-1,1,3,3,1,-1,-3,-3,-1,1,3,-3,-1,1,3,-3,-1,1,3,-1,-3,1,3,1,1,1,
            -1,-1,-1,-3,-3,3,3,-3,-3,-3,-3,-3,3,3,1,1,-1,-1 };
    static double as[63] = { 4.4844e-40,4.4356e-40,2.9345e-40,2.885e-40,
            1.6441e-40,1.5899e-40,7.2882e-41,6.7748e-41,1.0378e-41,1.3041e-42,
            1.5006e-41,1.537e-41,1.6139e-41,1.7143e-41,1.9985e-41,2.0169e-41,
            2.0994e-41,2.2094e-41,1.636e-41,1.6281e-41,1.6714e-41,1.7326e-41,
            8.0425e-42,8.0862e-42,8.0093e-42,8.1366e-42,2.4471e-42,2.5406e-42,
            2.6629e-42,2.8064e-42,4.6227e-42,4.715e-42,4.8513e-42,5.0133e-42,
            3.9968e-42,3.984e-42,3.981e-42,3.9687e-42,1.1806e-42,1.3458e-42,
            3.8746e-42,3.9219e-42,7.3334e-43,1.339e-42,1.3041e-42,7.1401e-43,
            1.3461e-42,6.5776e-43,6.9847e-43,1.3517e-42,7.5545e-43,1.3268e-42,
            6.9847e-43,1.3517e-42,7.464e-43,2.1322e-43,2.6037e-43,2.0823e-43,
            2.0632e-43,2.1067e-43,2.0531e-43,2.1218e-43,2.3006e-43 };
    static double bs[63] = { 4.3e-4,4.6e-4,8.3e-4,8.9e-4,.0017,.00186,
            .0041,.00457,0.,0.,9.99e-4,5.23e-4,1.49e-4,-1.68e-4,.001837,
            .001153,6.6e-4,2.54e-4,.003603,.002677,.002101,.001738,.00595,
            .006843,0.,.007035,.001025,6.42e-4,2.54e-4,-1.64e-4,.002342,
            .001975,.00164,.001328,.004943,.004999,.005461,.006839,0.,.010993,
            0.,0.,.001367,.005262,0.,.001601,.00451,0.,.001828,.004175,.04816,
            .007033,.001828,.004175,.009338,.003733,.008508,.006979,0.,
            .005035,0.,.004169,0. };
    static double twopic = 1.88365183e11;
    static double pi = 3.141592654;

    /* System generated locals */
    int s__1;
    double d__1;

    /* Local variables */
    double alfa;
    int nnii, nsol2;
    double a, b;
    int i__, l, n;
    double stoke, stoki, am, pf;
    int lp;
    double rm;
    int nr, iv;
    double stokip;
    int ivp;
    extern double clebsqr_(int *, int *, int *);
    extern /* Subroutine */ int profile_(double *, double *);


#define eb_ref(a_1,a_2) eb[(a_2)*41 + a_1 - 42]



/*     COMMON/APP3/SLIT,DX,NSRI,WNRMAX3,NS,NSRIUP */


/*          STORED VALUES */
    /* Parameter adjustments */
    --rsi;

    /* Function Body */


/*     EB(I,K) - BOUND ENERGIES */
/*     AM =  (MTX.EL. (L,BETA,L') )**2 */
/*     M(L,L',V,V') OF PAPER (*) ARE TO BE CORRECTED: */
/*     M(L,L',V,V') = AM * (2L+1) * C(L,3,L')**2 */
/*     NSRI - HOW MANY POINTS FOR B-B SPECTRAL FUNCTION TO BE GIVEN */
/*     WNRMAX3 - THE FREQUENCY RANGE OF B-B CONTRIBUTION */
/*     SLIT- THE HALFWIDTH OF THE SPECTRAL PROFILE CONVOLUTED WITH */
/*     B-B SPECTRUM, IN [CM-1]. */
/*       A,B, COEFFICIENTS , EQ. 7, A.BORYSOW, L.FROMMHOLD, */
/*       AP. J. VOL.311, 1043-1057, (1986) */

    nsri = 190;
    wnrmax3 = 45.;
    nsriup = (nsri << 1) + 1;
    dx = wnrmax3 / (double) nsri;
    ns = (int) (slit / dx);

    for (i__ = 1; i__ <= 401; ++i__) {
/* L300: */
        rsibb[i__ - 1] = 0.;
    }

    alfa = 1. / (*temp * .69519);
    rm = 2.32498211e-23;
/*     RM - REDUCED MASS FOR N2-N2 */

    d__1 = rm * 1.380662e-16 * *temp * 2. * pi / 4.3906208382975998e-53;
    pf = pow(d__1, c_b186);
/*       SCALE DOWN BY 1.D60 */
    pf *= 1e-60;

    nr = 0;
L555:
    ++nr;
    ldelvi = ldelvis[nr - 1];
    ivi = ivis[nr - 1];
    ivip = ivips[nr - 1];
    ldelel = ldelels[nr - 1];
    a = as[nr - 1];
    b = bs[nr - 1];
/*     WRITE (6,334) LDELVI,IVI,IVIP, LDELEL,A,B */
/* L334: */

/*       LDELVI=DELTA(V)=V'-V */
/*       IVI = V; IVIP = V' */
/*       LDELEL = DELTA(L) = L'-L */

    iv = ivi + 1;
    ivp = ivip + 1;
/*       THESE ARE ENERGY COLUMNS (V, V') */

    nnii = niv[iv - 1];

    s__1 = nnii;
    for (l = 1; l <= s__1; ++l) {
/*       LOOP OVER INITIAL L-VALUES... */

        am = a * exp(-b * (double) ((l - 1) * l));
/*       L - NUMBER OF ROW, (L-1) - ROTATIONAL LEVEL */
        lp = l + ldelel;
        ll = l - 1;
        llp = lp - 1;
/*       LL,LLP ARE INITIAL L AND FINAL L' ANGULAR MOMENTUM QUANTUM NUMBERS */

        if (lp > niv[ivp - 1] || lp < 1) {
            goto L20;
        }
        if (eb_ref(lp, ivp) == 0.) {
            goto L20;
        }
        if (eb_ref(l, iv) == 0.) {
            goto L20;
        }
        stoke = eb_ref(lp, ivp) - eb_ref(l, iv);

        stoki = am * exp(-alfa * eb_ref(l, iv)) / pf * (double) ((ll << 1)
                 + 1) * clebsqr_(&ll, &cs__3, &llp);

        profile_(&stoke, &stoki);
        if (stoki > 0.) {
            ++nlines;
        }

        stokip = am * exp(-alfa * eb_ref(lp, ivp)) / pf * (double) ((llp 
                << 1) + 1) * clebsqr_(&llp, &cs__3, &ll);

        d__1 = -stoke;
        profile_(&d__1, &stokip);
        if (stokip > 0.) {
            ++nlines;
        }

L20:
        ;
    }
    if (nr == 63) {
        goto L56;
    }
    goto L555;
L56:

/*     32 ENTRIES FOR (3220)+(3202) IN TABLE 6, 63 IN ALL: */
/*     DATA EXPANDED AND INCLUDE NOW ALL POSSIBLE B-B TRANSITIONS */

    s__1 = nsriup;
    for (n = 1; n <= s__1; ++n) {
/* L90: */
        rsibb[n - 1] = rsibb[n - 1] / twopic / slit;
    }

    *nsol = nsri + 1;
    nsol2 = *nsol + 1;
/*     RSI - CONTRIBUTION FOR POSITIVE FREQUENCY SHIFTS */

    s__1 = *nsol;
    for (i__ = 1; i__ <= s__1; ++i__) {
/* L22: */
        rsi[i__] = rsibb[*nsol - 1 + i__ - 1];
    }

/*        PRINT 999, (RSI(I),I=1,NSOL) */
/* L999: */

    return 0;
} /* bound32_ */

#undef slit
#undef dx
#undef wnrmax3
#undef nsri
#undef ns
#undef nsriup
#undef eb
#undef niv
#undef nlines
#undef rsibb
#undef ldelvi
#undef ivi
#undef ivip
#undef ldelel
#undef ll
#undef llp


#undef eb_ref

#define slit (app3a_1.slit)
#define dx (app3a_1.dx)
#define wnrmax3 (app3a_1.wnrmax3)
#define nsri (app3b_1.nsri)
#define ns (app3b_1.ns)
#define nsriup (app3b_1.nsriup)
#define eb (energ_1.eb)
#define niv (energ_1.niv)
#define nlines (dimer_1.nlines)
#define rsibb (bl3_2.rsibb)

/* Subroutine */ int bound54_(double *temp, double *rsi, int *
        nsol)
{
    /* Initialized data */

    static int ldelvis[54] = { 0,0,0,0,0,0,0,0,0,0,0,0,1,1,1,1,1,1,1,1,1,
            1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,2,2,2,2,2,2,2,2,2,2,2,2,2,2,2,2,2 
            };
    static int ivis[54] = { 0,0,0,1,1,1,2,2,2,3,3,3,0,0,0,0,0,0,1,1,1,1,
            1,1,2,2,2,2,2,2,3,3,3,3,3,3,0,0,0,0,0,0,1,1,1,1,1,1,2,2,2,2,2,2 };
    static int ivips[54] = { 0,0,0,1,1,1,2,2,2,3,3,3,1,1,1,1,1,1,2,2,2,2,
            2,2,3,3,3,3,3,3,4,4,4,4,4,4,2,2,2,2,2,2,3,3,3,3,3,3,4,4,4,4,4,4 };
    static int ldelels[54] = { 1,3,5,1,3,5,1,3,5,1,3,5,-5,-3,-1,1,3,5,-5,
            -3,-1,1,3,5,-5,-3,-1,1,3,5,-5,-3,-1,1,3,5,-5,-3,-1,1,3,5,-5,-3,-1,
            1,3,5,-5,-3,-1,1,3,5 };
    static double as[54] = { 7.9332e-42,7.8207e-42,7.7235e-42,4.5815e-42,
            4.4834e-42,4.4059e-42,2.173e-42,2.0824e-42,2.025e-42,7.7222e-43,
            7.0351e-43,6.6815e-43,4.9611e-43,5.2232e-43,5.2979e-43,5.4652e-43,
            5.6827e-43,5.9277e-43,5.733e-43,6.062e-43,6.0862e-43,6.2104e-43,
            6.3809e-43,6.5698e-43,3.9501e-43,4.1599e-43,4.1033e-43,4.1097e-43,
            4.1339e-43,4.153e-43,1.5858e-43,1.5976e-43,1.5478e-43,1.5066e-43,
            1.4554e-43,1.3848e-43,9.9241e-44,1.0109e-43,1.0396e-43,1.0758e-43,
            1.1176e-43,1.1636e-43,1.646e-43,1.647e-43,1.6617e-43,1.6837e-43,
            1.7085e-43,1.7327e-43,1.1797e-43,1.1593e-43,1.1405e-43,1.1174e-43,
            1.0853e-43,1.0401e-43 };
    static double bs[54] = { 6.12e-4,6.35e-4,6.77e-4,.001137,.001201,
            .001341,.00229,.002449,.00287,.005426,.005876,.00745,.001,8.83e-4,
            6.09e-4,3.92e-4,2.07e-4,3.7e-5,.001625,.001624,.001305,.001084,
            9.27e-4,8.21e-4,.002978,.003273,.002994,.002954,.003153,.003668,
            .005799,.006423,.006733,.00796,.010937,.019179,.001229,9.93e-4,
            7.67e-4,5.43e-4,3.09e-4,5.1e-5,.002456,.0023,.00221,.002193,
            .002273,.002506,.004556,.004825,.005454,.006725,.009431,.016672 };
    static double twopic = 1.88365183e11;
    static double pi = 3.141592654;

    /* System generated locals */
    int s__1;
    double d__1;

    /* Local variables */
    double alfa;
    int nnii, ivip, nsol2;
    double a, b;
    int i__, l, n;
    double stoke, stoki, am, pf;
    int ll, lp;
    double rm;
    int nr, ldelel, iv, ldelvi;
    double stokip;
    int ivi, llp, ivp;
    extern double clebsqr_(int *, int *, int *);
    extern /* Subroutine */ int profile_(double *, double *);


#define eb_ref(a_1,a_2) eb[(a_2)*41 + a_1 - 42]



/*     COMMON/APP3/SLIT,DX,NSRI,WNRMAX3,NS,NSRIUP */
/*          STORED VALUES */

/* TKS     THIS DATA STRUCTURE HAS 55 ENTRIES AND NOT 54!! */
/* TKS      DATA LDELVIS /0,0,0,0,0,0,0,0,0,0,0,0,1,1,1,1,1,1,1,1, */
/* TKS     &              1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,2,2,2, */
/* TKS     &              2,2,2,2,2,2,2,2,2,2,2,2,2,2,2/ */
/* TKS  WE HAVE SSKIPPED THE LAST "2" IN THIS DATA STATEMENT */
    /* Parameter adjustments */
    --rsi;

    /* Function Body */








    nsri = 190;
    wnrmax3 = 47.;
    nsriup = (nsri << 1) + 1;
    dx = wnrmax3 / (double) nsri;
    ns = (int) (slit / dx);

    for (i__ = 1; i__ <= 401; ++i__) {
/* L300: */
        rsibb[i__ - 1] = 0.;
    }
    alfa = 1. / (*temp * .69519);
    rm = 2.32498211e-23;
/*     RM - REDUCED MASS FOR N2-N2 */

    d__1 = rm * 1.380662e-16 * *temp * 2. * pi / 4.3906208382975998e-53;
    pf = pow(d__1, c_b186);
/*       SCALE DOWNWARD BY 1.D60 */
    pf *= 1e-60;

    nr = 0;
L555:
    ++nr;
    ldelvi = ldelvis[nr - 1];
    ivi = ivis[nr - 1];
    ivip = ivips[nr - 1];
    ldelel = ldelels[nr - 1];
    a = as[nr - 1];
    b = bs[nr - 1];
/*       WRITE (6,334) LDELVI,IVI,IVIP, LDELEL,A,B */
/* L334: */
/*       LDELVI=DELTA(V)=V'-V */
/*       IVI = V */
/*       LDELEL = DELTA(L) = L'-L */

    iv = ivi + 1;
    ivp = ivip + 1;
    nnii = niv[iv - 1];
    s__1 = nnii;
    for (l = 1; l <= s__1; ++l) {
        am = a * exp(-b * (double) (l * (l + 1)));
        lp = l + ldelel;
        ll = l - 1;
        llp = lp - 1;
        if (lp > niv[ivp - 1] || lp < 1) {
            goto L20;
        }
        if (eb_ref(lp, ivp) == 0.) {
            goto L20;
        }
        if (eb_ref(l, iv) == 0.) {
            goto L20;
        }

        stoke = eb_ref(lp, ivp) - eb_ref(l, iv);
        stoki = am * exp(-alfa * eb_ref(l, iv)) / pf * (double) ((ll << 1)
                 + 1) * clebsqr_(&ll, &cs__5, &llp);
        profile_(&stoke, &stoki);
        if (stoki > 0.) {
            ++nlines;
        }
        stokip = am * exp(-alfa * eb_ref(lp, ivp)) / pf * (double) ((llp 
                << 1) + 1) * clebsqr_(&llp, &cs__5, &ll);
        d__1 = -stoke;
        profile_(&d__1, &stokip);
        if (stokip > 0.) {
            ++nlines;
        }
L20:
        ;
    }
    if (nr == 54) {
        goto L56;
    }

    goto L555;
L56:
/*       54 ENTRIES FOR (5440)=(5404) IN TABLE 6 */

    s__1 = nsriup;
    for (n = 1; n <= s__1; ++n) {
/* L90: */
        rsibb[n - 1] = rsibb[n - 1] / twopic / slit;
    }

    *nsol = nsri + 1;
    nsol2 = *nsol + 1;

    s__1 = *nsol;
    for (i__ = 1; i__ <= s__1; ++i__) {
/* L22: */
        rsi[i__] = rsibb[*nsol - 1 + i__ - 1];
    }

/*     PRINT 999, (RSI(I),I=1,NSOL) */
/* L999: */

    return 0;
} /* bound54_ */

#undef slit
#undef dx
#undef wnrmax3
#undef nsri
#undef ns
#undef nsriup
#undef eb
#undef niv
#undef nlines
#undef rsibb


#undef eb_ref


double clebsqr_0_(int n__, int *l, int *lambda, int *lp)
{
    /* System generated locals */
    int s__1, s__2;
    double ret_val, d__1;

    /* Local variables */
    extern double fctl_(int *);
    double f;
    int i__;
    double p;
    int i0, i1;
    double fc;

/*     SQUARE OF CLEBSCH-GORDAN COEFFICIENT (L,LAMBDA,0,0;LP,0) */
/*     FOR INTEGER ARGUMENTS ONLY */
/*     NOTE THAT LAMBDA SHOULD BE SMALL, MAYBE @10 OR SO. */


    switch(n__) {
        case 1: goto L_threej2;
        }

    fc = (double) ((*lp << 1) + 1);
    goto L2;


L_threej2:
/*     THIS ENTRY RETURNS THE SQUARED 3-J SYMBOL   L LAMBDA LP */
/*                                                 0    0    0 */
/*     INSTEAD OF THE CLEBSCH-GORDAN COEFFICIENT */
/*     (LIMITATION TO INTEGER ARGUMENTS ONLY) */

/*     NOTE THAT THE THREE-J SYMBOLS ARE COMPLETELY SYMMETRIC IN THE */
/*     ARGUMENTS. IT WOULD BE ADVANTAGEOUS TO REORDER THE INPUT ARGUMENT */
/*     LIST SO THAT LAMBDA BECOMES THE SMALLEST OF THE 3 ARGUMENTS. */
    fc = 1.;
L2:
    ret_val = 0.;
    if (*l + *lambda < *lp || *lambda + *lp < *l || *l + *lp < *lambda) {
        return ret_val;
    }
    if ((*l + *lp + *lambda) % 2 != 0) {
        return ret_val;
    }
    if (*l < 0 || *lp < 0 || *lambda < 0) {
        return ret_val;
    }
    f = 1. / (double) (*l + *lp + 1 - *lambda);
    if (*lambda == 0) {
        goto L22;
    }
    i1 = (*l + *lp + *lambda) / 2;
    i0 = (*l + *lp - *lambda) / 2 + 1;
    s__1 = i1;
    for (i__ = i0; i__ <= s__1; ++i__) {
/* L20: */
        f = f * (double) i__ / (double) ((i__ << 1) + 1 << 1);
    }
L22:
    s__1 = *lambda + *l - *lp;
    s__2 = *lambda + *lp - *l;
    p = fc * f * fctl_(&s__1) * fctl_(&s__2);
    s__1 = (*lambda + *l - *lp) / 2;
    s__2 = (*lambda + *lp - *l) / 2;
/* Computing 2nd power */
    d__1 = fctl_(&s__1) * fctl_(&s__2);
    ret_val = p / (d__1 * d__1);
    return ret_val;
} /* clebsqr_ */

double clebsqr_(int *l, int *lambda, int *lp)
{
    return clebsqr_0_(0, l, lambda, lp);
    }

double threej2_(void)
{
    return clebsqr_0_(1, (int *)0, (int *)0, (int *)0);
    }

double fctl_(int *n)
{
    /* System generated locals */
    int s__1;
    double ret_val, d__1;

    /* Local variables */
    int i__, j;
    double z__;



    ret_val = 1.;
    if (*n <= 1) {
        return ret_val;
    }
    if (*n > 15) {
        goto L20;
    }
    j = 1;
    s__1 = *n;
    for (i__ = 2; i__ <= s__1; ++i__) {
/* L10: */
        j *= i__;
    }
    ret_val = (double) j;
    return ret_val;
L20:
    z__ = (double) (*n + 1);
    d__1 = z__ - .5;
    ret_val = exp(-z__) * pow(z__, d__1) * ((((-2.294720936e-4 / z__ - 
            .00268132716) / z__ + .003472222222) / z__ + .08333333333) / z__ 
            + 1.) * 2.506628274631;
    return ret_val;
} /* fctl_ */
#define ik1k0 (k1k0_1.ik1k0)

double bgama_(double *fnu, double *t1, double *t2, double 
        *eps, double *t3, double *t4, double *temp)
{
    /* Initialized data */

    static double pi = 3.1415926535898;
    static double clight = 29979245800.;
    static double hbar = 1.0545887e-27;
    static double boltz = 1.380662e-16;

    /* System generated locals */
    double ret_val, d__1, d__2, d__3, d__4;

    /* Local variables */
    double omega, z__, k0, t0, bgambc, zp, xk1;

/*     SPECTRAL FUNCTION "EBC", FOR REFERENCE: */
/*     SEE "PHENOMENA INDUCED BY INTERMOLECULAR INTERACTIONS", */
/*     ED. G. BIRNBAUM; J. BORYSOW AND L. FROMMHOLD, P.67, (1985) */
/*       ============================================ */


/*       IF IK1K0=1 ONLY B-C; EBC OTHERWISE */

    omega = 2. * pi * clight * *fnu;
    t0 = hbar / (boltz * 2. * *temp);
/* Computing 2nd power */
    d__1 = omega * *t1;
    z__ = sqrt((d__1 * d__1 + 1.) * (*t2 * *t2 + t0 * t0)) / *t1;
    if (z__ - 2. <= 0.) {
        goto L10;
    } else {
        goto L12;
    }
L10:
/* Computing 2nd power */
    d__2 = z__ / 3.75;
    d__1 = d__2 * d__2;
/* Computing 2nd power */
    d__4 = z__ / 2.;
    d__3 = d__4 * d__4;
    xk1 = z__ * z__ * log(z__ / 2.) * ((((((3.2411e-4 * d__1 + .00301532) * 
            d__1 + .02658733) * d__1 + .15084934) * d__1 + .51498869) * d__1 
            + .87890594) * d__1 + .5) + ((((((-4.686e-5 * d__3 - .00110404) * 
            d__3 - .01919402) * d__3 - .18156897) * d__3 - .67278579) * d__3 
            + .15443144) * d__3 + 1.);
    goto L20;
L12:
    d__1 = 2. / z__;
    xk1 = sqrt(z__) * exp(-z__) * ((((((-6.8245e-4 * d__1 + .00325614) * d__1 
            - .00780353) * d__1 + .01504268) * d__1 - .0365562) * d__1 + 
            .23498619) * d__1 + 1.25331414);
L20:
/* Computing 2nd power */
    d__1 = *t1 * omega;
    bgambc = *t1 / pi * exp(*t2 / *t1 + t0 * omega) * xk1 / (d__1 * d__1 + 1.)
            ;
    if (ik1k0 == 1) {
        goto L55;
    }
/* Computing 2nd power */
    d__1 = omega * *t4;
    zp = sqrt((d__1 * d__1 + 1.) * (*t3 * *t3 + t0 * t0)) / *t4;
    if (zp - 2. <= 0.) {
        goto L22;
    } else {
        goto L24;
    }
L22:
/* Computing 2nd power */
    d__2 = zp / 3.75;
    d__1 = d__2 * d__2;
/* Computing 2nd power */
    d__4 = zp / 2.;
    d__3 = d__4 * d__4;
    k0 = -log(zp / 2.) * ((((((.0045813 * d__1 + .0360768) * d__1 + .2659732) 
            * d__1 + 1.2067492) * d__1 + 3.0899424) * d__1 + 3.5156229) * 
            d__1 + 1.) + ((((((7.4e-6 * d__3 + 1.075e-4) * d__3 + .00262698) *
             d__3 + .0348859) * d__3 + .23069756) * d__3 + .4227842) * d__3 - 
            .57721566);
    goto L30;
L24:
    d__1 = 2. / zp;
    k0 = exp(-zp) * ((((((5.3208e-4 * d__1 - .0025154) * d__1 + .00587872) * 
            d__1 - .01062446) * d__1 + .02189568) * d__1 - .07832358) * d__1 
            + 1.25331414) / sqrt(zp);
L30:
    ret_val = (bgambc + *eps * (*t3 / pi) * exp(*t3 / *t4 + t0 * omega) * k0) 
            / (*eps + 1.);
    goto L66;
L55:
    ret_val = bgambc;
L66:
    return ret_val;
} /* bgama_ */

#undef ik1k0


/* Subroutine */ int spline_0_(int n__, int *l, int *m, int *k,
         double *eps, double *x, double *y, double *t, 
        double *ss, double *si, int *nr, double *s2)
{
    /* System generated locals */
    int s__1, s__2;
    double d__1, d__2;

    /* Local variables */
    double epsi, prod, h__;
    int i__, j, n;
    double w, omega;
    int n1;
    double s3;
    int ic;
    double sm, delsqs, ht1, ht2, ss2, yp1, eta, ypn;



/*     SPLINE INTERPOLATION AND QUADRATURE, THIRD ORDER AFTER GREVILLE. */
/*     INPUT ARGUMENTS L...Y, OUTPUT SS...NR. */
/*     L DATA POINTS X(1), Y(1) ... X(L),Y(L) */
/*     EPS=ERROR CRITERION, TYPICALLY EPS=1.D-5 FOR 5 DECI. PLACES ACCURA */
/*     M ARGUMENTS T(1)..T(M) FOR WHICH FUNCTION VALUES SS(1)..SS(M), FOR */
/*     K=0; OR FIRST OR SECOND DERIVATIVE FOR K=1 OR -1, RESPECTIVELY. */
/*     NOTE THAT M HAS TO BE AT LEAST EQUAL TO 1. */
/*     SI=INTEGRAL (OVER WHOLE INTERVAL) FOR K=2 ONLY. */
/*     FOR 'NATURAL' SPLINE FUNCTIONS, S2(1)=S2(L)=0. MUST BE INPUT*NOTE* */
/*     N0 INDICATES THE NUMBER OF OUT-OF-RANGE CALLS. X(1)<T(I)<X(L) */
/*     EXTRAPOLATE WITH CAUTION. (ASSUMPTION D2Y/DX2 = 0.) */
/*     S2(I) IS THE 2ND DERIVATIVE AT X=X(I) AND IS COMPUTED INTERNALLY. */
/*     DIMENSION X(L),Y(L),T(M),SS(M),S2(L) */

    /* Parameter adjustments */
    --x;
    --y;
    --t;
    --ss;
    --s2;

    /* Function Body */
    switch(n__) {
        case 1: goto L_ixpolat;
        }

    n = *l;
    n1 = n - 1;
    *nr = 0;
/* L4: */
    s__1 = n1;
    for (i__ = 2; i__ <= s__1; ++i__) {
/* L52: */
        s__2 = i__ - 1;
        s2[i__] = 3. * ((y[i__ + 1] - y[i__]) / (x[i__ + 1] - x[i__]) - (y[
                s__2 + 1] - y[s__2]) / (x[s__2 + 1] - x[s__2])) / (x[i__ + 1] 
                - x[i__ - 1]) / 1.5;
    }
    omega = 1.0717968;
    ic = 0;
/*     'NATURAL' SPLINE FUNCTIONS OF THIRD ORDER. */
    s2[1] = 0.;
    s2[n] = 0.;
L5:
    eta = 0.;
    ++ic;
    sm = abs(s2[1]);
    s__2 = n;
    for (i__ = 2; i__ <= s__2; ++i__) {
        if ((d__1 = s2[i__], abs(d__1)) > sm) {
            sm = (d__2 = s2[i__], abs(d__2));
        }
/* L25: */
    }
    epsi = *eps * sm;
/* L6: */
    s__2 = n1;
    for (i__ = 2; i__ <= s__2; ++i__) {
/* L7: */
        s__1 = i__ - 1;
        w = (3. * ((y[i__ + 1] - y[i__]) / (x[i__ + 1] - x[i__]) - (y[s__1 + 
                1] - y[s__1]) / (x[s__1 + 1] - x[s__1])) / (x[i__ + 1] - x[
                i__ - 1]) - (x[i__] - x[i__ - 1]) * .5 / (x[i__ + 1] - x[i__ 
                - 1]) * s2[i__ - 1] - (.5 - (x[i__] - x[i__ - 1]) * .5 / (x[
                i__ + 1] - x[i__ - 1])) * s2[i__ + 1] - s2[i__]) * omega;
/* L8: */
        if (abs(w) - eta <= 0.) {
            goto L10;
        } else {
            goto L9;
        }
L9:
        eta = abs(w);
L10:
        s2[i__] += w;
    }
/* L13: */
    if (eta - epsi >= 0.) {
        goto L5;
    } else {
        goto L14;
    }
/*     ENTRY IXPOLAT */

L_ixpolat:
/*     THIS ENTRY USEFUL WHEN ITERATION PREVIOUSLY COMPLETED */

    n = *l;
    n1 = n - 1;
    *nr = 0;
    ic = -1;
L14:
    if (*k - 2 != 0) {
        goto L15;
    } else {
        goto L20;
    }
L15:
    s__2 = *m;
    for (j = 1; j <= s__2; ++j) {
/* L16: */
        i__ = 1;
/* L54: */
        if ((d__1 = t[j] - x[1]) < 0.) {
            goto L58;
        } else if (d__1 == 0) {
            goto L17;
        } else {
            goto L55;
        }
L55:
        if ((d__1 = t[j] - x[n]) < 0.) {
            goto L57;
        } else if (d__1 == 0) {
            goto L59;
        } else {
            goto L158;
        }
L56:
        if ((d__1 = t[j] - x[i__]) < 0.) {
            goto L60;
        } else if (d__1 == 0) {
            goto L17;
        } else {
            goto L57;
        }
L57:
        ++i__;
        goto L56;

L58:
        ++(*nr);
        ht1 = t[j] - x[1];
        ht2 = t[j] - x[2];
        yp1 = (y[cs__1 + 1] - y[cs__1]) / (x[cs__1 + 1] - x[cs__1]) + (x[1] - 
                x[2]) * (s2[1] * 2. + s2[2]) / 6.;
        if (*k < 0) {
            goto L72;
        } else if (*k == 0) {
            goto L70;
        } else {
            goto L71;
        }
L71:
        ss[j] = yp1 + ht1 * s2[1];
        goto L61;
L70:
        ss[j] = y[1] + yp1 * ht1 + s2[1] * ht1 * ht1 / 2.;
        goto L61;
L72:
        ss[j] = s2[i__];
        goto L61;
L158:
        ht2 = t[j] - x[n];
        ht1 = t[j] - x[n1];
        ++(*nr);
        ypn = (y[n1 + 1] - y[n1]) / (x[n1 + 1] - x[n1]) + (x[n] - x[n1]) * (
                s2[n1] + s2[n] * 2.) / 6.;
        if (*k < 0) {
            goto L82;
        } else if (*k == 0) {
            goto L80;
        } else {
            goto L81;
        }
L81:
        ss[j] = ypn + ht2 * s2[n];
        goto L61;
L80:
        ss[j] = y[n] + ypn * ht2 + s2[n] * ht2 * ht2 / 2.;
        goto L61;
L82:
        ss[j] = s2[n];
        goto L61;

L59:
        i__ = n;
L60:
        --i__;
L17:
        ht1 = t[j] - x[i__];
        ht2 = t[j] - x[i__ + 1];
        prod = ht1 * ht2;
        s3 = (s2[i__ + 1] - s2[i__]) / (x[i__ + 1] - x[i__]);
        ss2 = s2[i__] + ht1 * s3;
        delsqs = (s2[i__] + s2[i__ + 1] + ss2) / 6.;

        if (*k < 0) {
            goto L43;
        } else if (*k == 0) {
            goto L41;
        } else {
            goto L42;
        }
L41:
        ss[j] = y[i__] + ht1 * ((y[i__ + 1] - y[i__]) / (x[i__ + 1] - x[i__]))
                 + prod * delsqs;
        goto L61;
L42:
        ss[j] = (y[i__ + 1] - y[i__]) / (x[i__ + 1] - x[i__]) + (ht1 + ht2) * 
                delsqs + prod * s3 / 6.;
        goto L61;
L43:
        ss[j] = ss2;
L61:
        ;
    }
L20:
    *si = 0.;

    s__2 = n1;
    for (i__ = 1; i__ <= s__2; ++i__) {
        h__ = x[i__ + 1] - x[i__];
/* L62: */
/* Computing 3rd power */
        d__1 = h__;
        *si = *si + h__ * .5 * (y[i__] + y[i__ + 1]) - d__1 * (d__1 * d__1) * 
                (s2[i__] + s2[i__ + 1]) / 24.;
    }

    if (*k == 2) {
        *nr = ic;
    }

    return 0;
} /* spline_ */

/* Subroutine */ int spline_(int *l, int *m, int *k, 
        double *eps, double *x, double *y, double *t, 
        double *ss, double *si, int *nr, double *s2)
{
    return spline_0_(0, l, m, k, eps, x, y, t, ss, si, nr, s2);
    }

/* Subroutine */ int ixpolat_(int *l, int *m, int *k, 
        double *eps, double *x, double *y, double *t, 
        double *ss, double *si, int *nr, double *s2)
{
    return spline_0_(1, l, m, k, eps, x, y, t, ss, si, nr, s2);
    }


// ---------------------- end of Borysow N2N2 F77 code -------------------------


// ---------------------- begin of monortm CKD F77 code -------------------------


/* Common Block Declarations */

struct fh2oa_1_ {
    double fh2o[2003];
};

#define fh2oa_1 (*(struct fh2oa_1_ *) &fh2oa_)

struct fh2ob_1_ {
    double v1, v2, dv;
    int nptfh2o;
};
struct fh2ob_2_ {
    double v1, v2, dv;
    int npts;
};

#define fh2ob_1 (*(struct fh2ob_1_ *) &fh2ob_)
#define fh2ob_2 (*(struct fh2ob_2_ *) &fh2ob_)

struct sh2oa_1_ {
    double swv296[2003];
};

#define sh2oa_1 (*(struct sh2oa_1_ *) &sh2oa_)

struct sh2ob_1_ {
    double v1, v2, dv;
    int nptslfwv;
};
struct sh2ob_2_ {
    double v1, v2, dv;
    int npts;
};

#define sh2ob_1 (*(struct sh2ob_1_ *) &sh2ob_)
#define sh2ob_2 (*(struct sh2ob_2_ *) &sh2ob_)

struct s260a_1_ {
    double swv260[2003];
};

#define s260a_1 (*(struct s260a_1_ *) &s260a_)

struct s260b_1_ {
    double v1___, v2___, dv___;
    int nptslfwv___;
};
struct s260b_2_ {
    double v1, v2, dv;
    int npts;
};

#define s260b_1 (*(struct s260b_1_ *) &s260b_)
#define s260b_2 (*(struct s260b_2_ *) &s260b_)

struct consts_1_ {
    double pi, planck, boltz, clight, avogad, alosmt, gascon, radcn1, 
            radcn2;
};

#define consts_1 (*(struct consts_1_ *) &consts_)

/* Initialized data */

struct s_fh2oa_ {
    double e_1[2003];
    } fh2oa_ = { {.012859, .011715, .011038, .011715, .012859, .015326, 
            .016999, .018321, .019402, .01957, .019432, .017572, .01676, 
            .01548, .013984, .012266, .010467, .0094526, .0080485, .0069484, 
            .0061416, .0050941, .0044836, .0038133, .0034608, .0031487, 
            .0024555, .0020977, .0017266, .001492, .0012709, 9.8081e-4, 
            8.5063e-4, 6.8822e-4, 5.3809e-4, 4.4679e-4, 3.3774e-4, 2.7979e-4, 
            2.1047e-4, 1.6511e-4, 1.2993e-4, 9.3033e-5, 7.436e-5, 5.6428e-5, 
            4.5442e-5, 3.4575e-5, 2.7903e-5, 2.1374e-5, 1.6075e-5, 1.3022e-5, 
            1.0962e-5, 8.5959e-6, 6.9125e-6, 5.3808e-6, 4.3586e-6, 3.6394e-6, 
            2.9552e-6, 2.3547e-6, 1.8463e-6, 1.6036e-6, 1.3483e-6, 1.1968e-6, 
            1.0333e-6, 8.4484e-7, 6.7195e-7, 5.0947e-7, 4.2343e-7, 3.4453e-7, 
            2.783e-7, 2.3063e-7, 1.9951e-7, 1.7087e-7, 1.4393e-7, 1.2575e-7, 
            1.075e-7, 8.2325e-8, 5.7524e-8, 4.4482e-8, 3.8106e-8, 3.4315e-8, 
            2.9422e-8, 2.5069e-8, 2.2402e-8, 1.9349e-8, 1.6152e-8, 1.2208e-8, 
            8.966e-9, 7.1322e-9, 6.1028e-9, 5.2938e-9, 4.535e-9, 3.4977e-9, 
            2.9511e-9, 2.4734e-9, 2.0508e-9, 1.8507e-9, 1.6373e-9, 1.5171e-9, 
            1.3071e-9, 1.2462e-9, 1.2148e-9, 1.259e-9, 1.3153e-9, 1.3301e-9, 
            1.4483e-9, 1.6944e-9, 2.0559e-9, 2.2954e-9, 2.6221e-9, 3.2606e-9, 
            4.2392e-9, 5.2171e-9, 6.2553e-9, 8.2548e-9, 9.5842e-9, 1.128e-8, 
            1.3628e-8, 1.7635e-8, 2.1576e-8, 2.4835e-8, 3.0014e-8, 3.8485e-8, 
            4.744e-8, 5.5202e-8, 7.0897e-8, 9.6578e-8, 1.3976e-7, 1.8391e-7, 
            2.3207e-7, 2.996e-7, 4.0408e-7, 5.926e-7, 7.8487e-7, 1.0947e-6, 
            1.4676e-6, 1.9325e-6, 2.6587e-6, 3.4534e-6, 4.4376e-6, 5.8061e-6, 
            7.0141e-6, 8.4937e-6, 1.0186e-5, 1.2034e-5, 1.3837e-5, 1.6595e-5, 
            1.9259e-5, 2.162e-5, 2.3681e-5, 2.7064e-5, 3.251e-5, 3.546e-5, 
            3.9109e-5, 4.2891e-5, 4.7757e-5, 5.0981e-5, 5.0527e-5, 4.8618e-5, 
            4.4001e-5, 3.7982e-5, 3.2667e-5, 2.7794e-5, 2.491e-5, 2.4375e-5, 
            2.7316e-5, 3.2579e-5, 3.5499e-5, 3.801e-5, 4.1353e-5, 4.3323e-5, 
            4.3004e-5, 3.979e-5, 3.7718e-5, 3.636e-5, 3.2386e-5, 2.7409e-5, 
            2.3626e-5, 2.0631e-5, 1.8371e-5, 1.5445e-5, 1.2989e-5, 1.1098e-5, 
            9.6552e-6, 8.0649e-6, 7.2365e-6, 5.9137e-6, 5.2759e-6, 4.886e-6, 
            4.1321e-6, 3.5918e-6, 2.764e-6, 2.4892e-6, 2.1018e-6, 1.7848e-6, 
            1.5855e-6, 1.3569e-6, 1.1986e-6, 9.4693e-7, 7.4097e-7, 6.3443e-7, 
            4.8131e-7, 4.0942e-7, 3.3316e-7, 2.8488e-7, 2.3461e-7, 1.7397e-7, 
            1.4684e-7, 1.0953e-7, 8.5396e-8, 6.9261e-8, 5.4001e-8, 4.543e-8, 
            3.2791e-8, 2.5995e-8, 2.0225e-8, 1.571e-8, 1.3027e-8, 1.0229e-8, 
            8.5277e-9, 6.5249e-9, 5.0117e-9, 3.9906e-9, 3.2332e-9, 2.7847e-9, 
            2.457e-9, 2.3359e-9, 2.0599e-9, 1.8436e-9, 1.6559e-9, 1.491e-9, 
            1.2794e-9, 9.8229e-10, 8.0054e-10, 6.0769e-10, 4.5646e-10, 
            3.3111e-10, 2.4428e-10, 1.8007e-10, 1.3291e-10, 9.7974e-11, 
            7.8271e-11, 6.3833e-11, 5.4425e-11, 4.6471e-11, 4.0209e-11, 
            3.5227e-11, 3.1212e-11, 2.884e-11, 2.7762e-11, 2.7935e-11, 
            3.2012e-11, 3.9525e-11, 5.0303e-11, 6.8027e-11, 9.3954e-11, 
            1.2986e-10, 1.8478e-10, 2.5331e-10, 3.4827e-10, 4.6968e-10, 
            6.238e-10, 7.9106e-10, 1.0026e-9, 1.2102e-9, 1.4146e-9, 1.6154e-9,
             1.751e-9, 1.8575e-9, 1.8742e-9, 1.87e-9, 1.8582e-9, 1.9657e-9, 
            2.1204e-9, 2.0381e-9, 2.0122e-9, 2.0436e-9, 2.1213e-9, 2.0742e-9, 
            1.987e-9, 2.0465e-9, 2.1556e-9, 2.2222e-9, 2.1977e-9, 2.1047e-9, 
            1.9334e-9, 1.7357e-9, 1.5754e-9, 1.4398e-9, 1.4018e-9, 1.5459e-9, 
            1.7576e-9, 2.1645e-9, 2.948e-9, 4.4439e-9, 5.8341e-9, 8.0757e-9, 
            1.1658e-8, 1.6793e-8, 2.2694e-8, 2.9468e-8, 3.9278e-8, 5.2145e-8, 
            6.4378e-8, 7.7947e-8, 8.5321e-8, 9.7848e-8, 1.0999e-7, 1.1489e-7, 
            1.2082e-7, 1.2822e-7, 1.4053e-7, 1.5238e-7, 1.5454e-7, 1.5018e-7, 
            1.4048e-7, 1.2359e-7, 1.0858e-7, 9.3486e-8, 8.1638e-8, 7.769e-8, 
            8.4625e-8, 1.0114e-7, 1.143e-7, 1.2263e-7, 1.3084e-7, 1.338e-7, 
            1.3573e-7, 1.3441e-7, 1.2962e-7, 1.2638e-7, 1.1934e-7, 1.1371e-7, 
            1.0871e-7, 9.8843e-8, 9.1877e-8, 9.105e-8, 9.3213e-8, 9.2929e-8, 
            1.0155e-7, 1.1263e-7, 1.237e-7, 1.3636e-7, 1.54e-7, 1.7656e-7, 
            2.1329e-7, 2.3045e-7, 2.5811e-7, 2.9261e-7, 3.4259e-7, 4.077e-7, 
            4.8771e-7, 5.8081e-7, 7.2895e-7, 8.7482e-7, 1.0795e-6, 1.3384e-6, 
            1.7208e-6, 2.0677e-6, 2.5294e-6, 3.1123e-6, 3.79e-6, 4.7752e-6, 
            5.6891e-6, 6.6261e-6, 7.6246e-6, 8.773e-6, 9.6672e-6, 1.098e-5, 
            1.1287e-5, 1.167e-5, 1.1635e-5, 1.1768e-5, 1.2039e-5, 1.2253e-5, 
            1.3294e-5, 1.4005e-5, 1.3854e-5, 1.342e-5, 1.3003e-5, 1.2645e-5, 
            1.1715e-5, 1.1258e-5, 1.1516e-5, 1.2494e-5, 1.3655e-5, 1.4931e-5, 
            1.4649e-5, 1.3857e-5, 1.312e-5, 1.1791e-5, 1.0637e-5, 8.276e-6, 
            6.5821e-6, 5.1959e-6, 4.0158e-6, 3.0131e-6, 2.0462e-6, 1.4853e-6, 
            1.0365e-6, 7.3938e-7, 4.9752e-7, 3.4148e-7, 2.4992e-7, 1.8363e-7, 
            1.4591e-7, 1.138e-7, 9.0588e-8, 7.3697e-8, 6.0252e-8, 5.1868e-8, 
            4.266e-8, 3.6163e-8, 3.2512e-8, 2.9258e-8, 2.4238e-8, 2.1209e-8, 
            1.6362e-8, 1.3871e-8, 1.2355e-8, 9.694e-9, 7.7735e-9, 6.2278e-9, 
            5.2282e-9, 4.3799e-9, 3.5545e-9, 2.7527e-9, 2.095e-9, 1.6344e-9, 
            1.2689e-9, 1.0403e-9, 8.488e-10, 6.3461e-10, 4.7657e-10, 
            3.522e-10, 2.7879e-10, 2.3021e-10, 1.6167e-10, 1.1732e-10, 
            8.9206e-11, 7.0596e-11, 5.831e-11, 4.4084e-11, 3.1534e-11, 
            2.5068e-11, 2.2088e-11, 2.2579e-11, 2.2637e-11, 2.5705e-11, 
            3.2415e-11, 4.6116e-11, 6.5346e-11, 9.4842e-11, 1.2809e-10, 
            1.8211e-10, 2.4052e-10, 3.027e-10, 3.5531e-10, 4.2402e-10, 
            4.673e-10, 4.7942e-10, 4.6813e-10, 4.5997e-10, 4.5788e-10, 
            4.0311e-10, 3.7367e-10, 3.3149e-10, 2.9281e-10, 2.5231e-10, 
            2.1152e-10, 1.9799e-10, 1.8636e-10, 1.9085e-10, 2.0786e-10, 
            2.2464e-10, 2.3785e-10, 2.5684e-10, 2.7499e-10, 2.6962e-10, 
            2.6378e-10, 2.6297e-10, 2.6903e-10, 2.7035e-10, 2.5394e-10, 
            2.5655e-10, 2.7184e-10, 2.9013e-10, 3.0585e-10, 3.0791e-10, 
            3.1667e-10, 3.4343e-10, 3.7365e-10, 4.0269e-10, 4.726e-10, 
            5.6584e-10, 6.9791e-10, 8.6569e-10, 1.0393e-9, 1.2067e-9, 
            1.5047e-9, 1.8583e-9, 2.2357e-9, 2.6498e-9, 3.2483e-9, 3.9927e-9, 
            4.6618e-9, 5.5555e-9, 6.6609e-9, 8.2139e-9, 1.0285e-8, 1.3919e-8, 
            1.8786e-8, 2.515e-8, 3.313e-8, 4.5442e-8, 6.337e-8, 9.0628e-8, 
            1.2118e-7, 1.5927e-7, 2.1358e-7, 2.7825e-7, 3.7671e-7, 4.4894e-7, 
            5.4442e-7, 6.224e-7, 7.3004e-7, 8.3384e-7, 8.7933e-7, 8.808e-7, 
            8.6939e-7, 8.6541e-7, 8.2055e-7, 7.7278e-7, 7.5989e-7, 8.6909e-7, 
            9.7945e-7, 1.0394e-6, 1.0646e-6, 1.1509e-6, 1.2017e-6, 1.1915e-6, 
            1.1259e-6, 1.1549e-6, 1.1938e-6, 1.2356e-6, 1.2404e-6, 1.1716e-6, 
            1.1149e-6, 1.0073e-6, 8.9845e-7, 7.6639e-7, 6.1517e-7, 5.0887e-7, 
            4.1269e-7, 3.2474e-7, 2.5698e-7, 1.8893e-7, 1.4009e-7, 1.034e-7, 
            7.7724e-8, 5.7302e-8, 4.2178e-8, 2.9603e-8, 2.1945e-8, 1.6301e-8, 
            1.2806e-8, 1.0048e-8, 7.897e-9, 6.1133e-9, 4.9054e-9, 4.1985e-9, 
            3.6944e-9, 3.2586e-9, 2.7362e-9, 2.3647e-9, 2.1249e-9, 1.8172e-9, 
            1.6224e-9, 1.5158e-9, 1.2361e-9, 1.0682e-9, 9.2312e-10, 7.922e-10,
             6.8174e-10, 5.6147e-10, 4.8268e-10, 4.1534e-10, 3.3106e-10, 
            2.8275e-10, 2.4584e-10, 2.0742e-10, 1.784e-10, 1.4664e-10, 
            1.239e-10, 1.0497e-10, 8.5038e-11, 6.7008e-11, 5.6355e-11, 
            4.3323e-11, 3.6914e-11, 3.2262e-11, 3.0749e-11, 3.0318e-11, 
            2.9447e-11, 2.9918e-11, 3.0668e-11, 3.1315e-11, 3.0329e-11, 
            2.8259e-11, 2.6065e-11, 2.3578e-11, 2.0469e-11, 1.6908e-11, 
            1.4912e-11, 1.1867e-11, 9.973e-12, 8.1014e-12, 6.7528e-12, 
            6.3133e-12, 5.8599e-12, 6.0145e-12, 6.5105e-12, 7.0537e-12, 
            7.4973e-12, 7.8519e-12, 8.5039e-12, 9.1995e-12, 1.0694e-11, 
            1.1659e-11, 1.2685e-11, 1.3087e-11, 1.3222e-11, 1.2634e-11, 
            1.1077e-11, 9.6259e-12, 8.3202e-12, 7.4857e-12, 6.8069e-12, 
            6.7496e-12, 7.3116e-12, 8.0171e-12, 8.6394e-12, 9.2659e-12, 
            1.0048e-11, 1.0941e-11, 1.2226e-11, 1.3058e-11, 1.5193e-11, 
            1.8923e-11, 2.3334e-11, 2.8787e-11, 3.6693e-11, 4.8295e-11, 
            6.426e-11, 8.8269e-11, 1.1865e-10, 1.5961e-10, 2.0605e-10, 
            2.7349e-10, 3.7193e-10, 4.8216e-10, 6.1966e-10, 7.715e-10, 
            1.0195e-9, 1.2859e-9, 1.6535e-9, 2.0316e-9, 2.3913e-9, 3.0114e-9, 
            3.7495e-9, 4.6504e-9, 5.9145e-9, 7.684e-9, 1.0304e-8, 1.301e-8, 
            1.6441e-8, 2.1475e-8, 2.5892e-8, 2.9788e-8, 3.382e-8, 4.0007e-8, 
            4.4888e-8, 4.5765e-8, 4.6131e-8, 4.6239e-8, 4.4849e-8, 4.0729e-8, 
            3.6856e-8, 3.6164e-8, 3.7606e-8, 4.1457e-8, 4.375e-8, 5.115e-8, 
            5.6054e-8, 6.1586e-8, 6.4521e-8, 6.6494e-8, 6.9024e-8, 6.8893e-8, 
            7.0901e-8, 6.976e-8, 7.1485e-8, 7.074e-8, 7.3764e-8, 7.6618e-8, 
            8.4182e-8, 9.3838e-8, 1.0761e-7, 1.2851e-7, 1.4748e-7, 1.8407e-7, 
            2.2109e-7, 2.6392e-7, 2.9887e-7, 3.4493e-7, 4.0336e-7, 4.3551e-7, 
            4.9231e-7, 5.0728e-7, 5.3781e-7, 5.3285e-7, 5.4496e-7, 5.5707e-7, 
            5.6944e-7, 6.1123e-7, 6.4317e-7, 6.4581e-7, 6.1999e-7, 6.0191e-7, 
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            3.933e-11, 4.4208e-11, 4.6431e-11, 5.1141e-11, 5.4108e-11, 
            5.8077e-11, 6.505e-11, 7.2126e-11, 8.1064e-11, 8.1973e-11, 
            8.1694e-11, 8.3081e-11, 8.024e-11, 7.9225e-11, 7.6256e-11, 
            7.8468e-11, 8.0041e-11, 8.1585e-11, 8.3485e-11, 8.3774e-11, 
            8.587e-11, 8.6104e-11, 8.8516e-11, 9.0814e-11, 9.2522e-11, 
            8.8913e-11, 7.8381e-11, 6.8568e-11, 5.6797e-11, 4.4163e-11, 
            3.2369e-11, 2.3259e-11, 1.6835e-11, 1.1733e-11, 8.5273e-12, 
            6.3805e-12, 4.8983e-12, 3.8831e-12, 3.261e-12, 2.8577e-12, 
            2.521e-12, 2.2913e-12, 2.0341e-12, 1.8167e-12, 1.6395e-12, 
            1.489e-12, 1.3516e-12, 1.2542e-12, 1.291e-12, 1.3471e-12, 
            1.4689e-12, 1.5889e-12, 1.6989e-12, 1.8843e-12, 2.0902e-12, 
            2.3874e-12, 2.7294e-12, 3.3353e-12, 4.0186e-12, 4.5868e-12, 
            5.2212e-12, 5.8856e-12, 6.5991e-12, 7.2505e-12, 7.6637e-12, 
            8.5113e-12, 9.4832e-12, 9.9678e-12, 1.0723e-11, 1.0749e-11, 
            1.138e-11, 1.1774e-11, 1.1743e-11, 1.2493e-11, 1.2559e-11, 
            1.2332e-11, 1.1782e-11, 1.1086e-11, 1.0945e-11, 1.1178e-11, 
            1.2083e-11, 1.3037e-11, 1.473e-11, 1.645e-11, 1.7403e-11, 
            1.7004e-11, 1.5117e-11, 1.3339e-11, 1.0844e-11, 8.0915e-12, 
            5.6615e-12, 3.7196e-12, 2.5194e-12, 1.6569e-12, 1.1201e-12, 
            8.2335e-13, 6.027e-13, 4.8205e-13, 4.1313e-13, 3.6243e-13, 
            3.2575e-13, 2.773e-13, 2.5292e-13, 2.3062e-13, 2.1126e-13, 
            2.1556e-13, 2.1213e-13, 2.2103e-13, 2.1927e-13, 2.0794e-13, 
            1.9533e-13, 1.6592e-13, 1.4521e-13, 1.1393e-13, 8.3772e-14, 
            6.2077e-14, 4.3337e-14, 2.7165e-14, 1.6821e-14, 9.5407e-15, 
            5.3093e-15, 3.032e-15, 1.7429e-15, 9.9828e-16, 5.6622e-16, 
            3.1672e-16, 1.7419e-16, 9.3985e-17, 4.9656e-17, 2.5652e-17, 
            1.2942e-17, 6.3695e-18, 3.0554e-18, 1.4273e-18, -0., -0., -0., 
            -0., -0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 
            0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 
            0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 
            0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 
            0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 
            0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 
            0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 
            0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 
            0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 
            0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 
            0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 
            0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.} };

struct s_fh2ob_ {
    double e_1[3];
    int e_2;
    } fh2ob_ = { {-20., 2e4, 10.}, 2003 };

struct s_sh2oa_ {
    double e_1[2003];
    } sh2oa_ = { {.11109, .10573, .10162, .10573, .11109, .12574, .13499, 
            .14327, .15065, .15164, .15022, .13677, .13115, .12253, .11271, 
            .1007, .087495, .080118, .06994, .062034, .056051, .047663, 
            .04245, .03669, .033441, .030711, .025205, .022113, .01888, 
            .016653, .014626, .012065, .010709, .0091783, .0077274, .0067302, 
            .0056164, .0049089, .0041497, .0035823, .0031124, .0026414, 
            .0023167, .0020156, .0017829, .0015666, .0013928, .0012338, 
            .0010932, 9.7939e-4, 8.8241e-4, 7.9173e-4, 7.1296e-4, 6.4179e-4, 
            5.8031e-4, 5.2647e-4, 4.7762e-4, 4.3349e-4, 3.9355e-4, 3.5887e-4, 
            3.2723e-4, 2.9919e-4, 2.7363e-4, 2.5013e-4, 2.2876e-4, 2.0924e-4, 
            1.9193e-4, 1.7618e-4, 1.6188e-4, 1.4891e-4, 1.3717e-4, 1.2647e-4, 
            1.1671e-4, 1.0786e-4, 9.9785e-5, 9.235e-5, 8.5539e-5, 7.9377e-5, 
            7.3781e-5, 6.8677e-5, 6.3993e-5, 5.9705e-5, 5.5788e-5, 5.2196e-5, 
            4.8899e-5, 4.5865e-5, 4.3079e-5, 4.0526e-5, 3.8182e-5, 3.6025e-5, 
            3.4038e-5, 3.2203e-5, 3.0511e-5, 2.8949e-5, 2.7505e-5, 2.617e-5, 
            2.4933e-5, 2.3786e-5, 2.2722e-5, 2.1736e-5, 2.0819e-5, 1.9968e-5, 
            1.9178e-5, 1.8442e-5, 1.776e-5, 1.7127e-5, 1.6541e-5, 1.5997e-5, 
            1.5495e-5, 1.5034e-5, 1.4614e-5, 1.423e-5, 1.3883e-5, 1.3578e-5, 
            1.3304e-5, 1.3069e-5, 1.2876e-5, 1.2732e-5, 1.2626e-5, 1.2556e-5, 
            1.2544e-5, 1.2604e-5, 1.2719e-5, 1.2883e-5, 1.3164e-5, 1.3581e-5, 
            1.4187e-5, 1.4866e-5, 1.5669e-5, 1.6717e-5, 1.8148e-5, 2.0268e-5, 
            2.2456e-5, 2.5582e-5, 2.9183e-5, 3.3612e-5, 3.9996e-5, 4.6829e-5, 
            5.5055e-5, 6.5897e-5, 7.536e-5, 8.7213e-5, 1.0046e-4, 1.1496e-4, 
            1.2943e-4, 1.5049e-4, 1.6973e-4, 1.8711e-4, 2.0286e-4, 2.2823e-4, 
            2.678e-4, 2.8766e-4, 3.1164e-4, 3.364e-4, 3.6884e-4, 3.9159e-4, 
            3.8712e-4, 3.7433e-4, 3.4503e-4, 3.1003e-4, 2.8027e-4, 2.5253e-4, 
            2.3408e-4, 2.2836e-4, 2.4442e-4, 2.7521e-4, 2.9048e-4, 3.0489e-4, 
            3.2646e-4, 3.388e-4, 3.3492e-4, 3.0987e-4, 2.9482e-4, 2.8711e-4, 
            2.6068e-4, 2.2683e-4, 1.9996e-4, 1.7788e-4, 1.6101e-4, 1.3911e-4, 
            1.2013e-4, 1.0544e-4, 9.4224e-5, 8.1256e-5, 7.3667e-5, 6.2233e-5, 
            5.5906e-5, 5.1619e-5, 4.514e-5, 4.0273e-5, 3.3268e-5, 3.0258e-5, 
            2.644e-5, 2.3103e-5, 2.0749e-5, 1.8258e-5, 1.6459e-5, 1.4097e-5, 
            1.2052e-5, 1.0759e-5, 9.14e-6, 8.1432e-6, 7.146e-6, 6.4006e-6, 
            5.6995e-6, 4.9372e-6, 4.4455e-6, 3.9033e-6, 3.474e-6, 3.1269e-6, 
            2.8059e-6, 2.5558e-6, 2.2919e-6, 2.0846e-6, 1.8983e-6, 1.7329e-6, 
            1.5929e-6, 1.4631e-6, 1.3513e-6, 1.2461e-6, 1.1519e-6, 1.0682e-6, 
            9.9256e-7, 9.2505e-7, 8.6367e-7, 8.0857e-7, 7.5674e-7, 7.0934e-7, 
            6.658e-7, 6.258e-7, 5.8853e-7, 5.5333e-7, 5.2143e-7, 4.9169e-7, 
            4.6431e-7, 4.3898e-7, 4.1564e-7, 3.9405e-7, 3.7403e-7, 3.5544e-7, 
            3.3819e-7, 3.2212e-7, 3.0714e-7, 2.9313e-7, 2.8003e-7, 2.6777e-7, 
            2.5628e-7, 2.4551e-7, 2.354e-7, 2.2591e-7, 2.1701e-7, 2.0866e-7, 
            2.0082e-7, 1.9349e-7, 1.8665e-7, 1.8027e-7, 1.7439e-7, 1.6894e-7, 
            1.64e-7, 1.5953e-7, 1.5557e-7, 1.5195e-7, 1.4888e-7, 1.4603e-7, 
            1.4337e-7, 1.4093e-7, 1.3828e-7, 1.3569e-7, 1.327e-7, 1.2984e-7, 
            1.2714e-7, 1.2541e-7, 1.2399e-7, 1.2102e-7, 1.1878e-7, 1.1728e-7, 
            1.1644e-7, 1.1491e-7, 1.1305e-7, 1.1235e-7, 1.1228e-7, 1.1224e-7, 
            1.1191e-7, 1.1151e-7, 1.1098e-7, 1.1068e-7, 1.1109e-7, 1.1213e-7, 
            1.1431e-7, 1.1826e-7, 1.2322e-7, 1.3025e-7, 1.4066e-7, 1.5657e-7, 
            1.7214e-7, 1.9449e-7, 2.2662e-7, 2.6953e-7, 3.1723e-7, 3.7028e-7, 
            4.4482e-7, 5.3852e-7, 6.2639e-7, 7.2175e-7, 7.7626e-7, 8.7248e-7, 
            9.6759e-7, 1.0102e-6, 1.062e-6, 1.1201e-6, 1.2107e-6, 1.2998e-6, 
            1.313e-6, 1.2856e-6, 1.235e-6, 1.1489e-6, 1.0819e-6, 1.012e-6, 
            9.4795e-7, 9.2858e-7, 9.806e-7, 1.0999e-6, 1.1967e-6, 1.2672e-6, 
            1.3418e-6, 1.3864e-6, 1.433e-6, 1.4592e-6, 1.4598e-6, 1.4774e-6, 
            1.4726e-6, 1.482e-6, 1.505e-6, 1.4984e-6, 1.5181e-6, 1.5888e-6, 
            1.685e-6, 1.769e-6, 1.9277e-6, 2.1107e-6, 2.3068e-6, 2.5347e-6, 
            2.8069e-6, 3.1345e-6, 3.5822e-6, 3.9051e-6, 4.3422e-6, 4.8704e-6, 
            5.5351e-6, 6.3454e-6, 7.269e-6, 8.2974e-6, 9.7609e-6, 1.1237e-5, 
            1.3187e-5, 1.5548e-5, 1.8784e-5, 2.1694e-5, 2.5487e-5, 3.0092e-5, 
            3.5385e-5, 4.2764e-5, 4.9313e-5, 5.58e-5, 6.2968e-5, 7.106e-5, 
            7.7699e-5, 8.7216e-5, 8.9335e-5, 9.2151e-5, 9.2779e-5, 9.4643e-5, 
            9.7978e-5, 1.0008e-4, 1.0702e-4, 1.1026e-4, 1.0828e-4, 1.055e-4, 
            1.0432e-4, 1.0428e-4, 9.898e-5, 9.4992e-5, 9.5159e-5, 1.0058e-4, 
            1.0738e-4, 1.155e-4, 1.1229e-4, 1.0596e-4, 1.0062e-4, 9.1742e-5, 
            8.4492e-5, 6.8099e-5, 5.6295e-5, 4.6502e-5, 3.8071e-5, 3.0721e-5, 
            2.3297e-5, 1.8688e-5, 1.483e-5, 1.2049e-5, 9.6754e-6, 7.9192e-6, 
            6.6673e-6, 5.6468e-6, 4.8904e-6, 4.2289e-6, 3.688e-6, 3.2396e-6, 
            2.8525e-6, 2.5363e-6, 2.2431e-6, 1.9949e-6, 1.7931e-6, 1.6164e-6, 
            1.4431e-6, 1.2997e-6, 1.1559e-6, 1.0404e-6, 9.43e-7, 8.4597e-7, 
            7.6133e-7, 6.8623e-7, 6.2137e-7, 5.6345e-7, 5.1076e-7, 4.6246e-7, 
            4.1906e-7, 3.8063e-7, 3.461e-7, 3.1554e-7, 2.8795e-7, 2.6252e-7, 
            2.3967e-7, 2.1901e-7, 2.0052e-7, 1.8384e-7, 1.6847e-7, 1.5459e-7, 
            1.4204e-7, 1.3068e-7, 1.2036e-7, 1.1095e-7, 1.0237e-7, 9.4592e-8, 
            8.753e-8, 8.1121e-8, 7.5282e-8, 6.9985e-8, 6.5189e-8, 6.0874e-8, 
            5.6989e-8, 5.353e-8, 5.0418e-8, 4.7745e-8, 4.5367e-8, 4.3253e-8, 
            4.1309e-8, 3.9695e-8, 3.8094e-8, 3.6482e-8, 3.4897e-8, 3.35e-8, 
            3.2302e-8, 3.0854e-8, 2.9698e-8, 2.8567e-8, 2.76e-8, 2.6746e-8, 
            2.5982e-8, 2.551e-8, 2.5121e-8, 2.4922e-8, 2.4909e-8, 2.5013e-8, 
            2.5216e-8, 2.5589e-8, 2.6049e-8, 2.6451e-8, 2.6978e-8, 2.7687e-8, 
            2.86e-8, 2.9643e-8, 3.0701e-8, 3.2058e-8, 3.3695e-8, 3.5558e-8, 
            3.7634e-8, 3.9875e-8, 4.2458e-8, 4.548e-8, 4.8858e-8, 5.2599e-8, 
            5.703e-8, 6.2067e-8, 6.7911e-8, 7.4579e-8, 8.1902e-8, 8.9978e-8, 
            9.987e-8, 1.1102e-7, 1.2343e-7, 1.3732e-7, 1.5394e-7, 1.7318e-7, 
            1.9383e-7, 2.1819e-7, 2.4666e-7, 2.8109e-7, 3.2236e-7, 3.776e-7, 
            4.4417e-7, 5.2422e-7, 6.1941e-7, 7.4897e-7, 9.2041e-7, 1.1574e-6, 
            1.4126e-6, 1.7197e-6, 2.1399e-6, 2.6266e-6, 3.3424e-6, 3.8418e-6, 
            4.514e-6, 5.0653e-6, 5.8485e-6, 6.5856e-6, 6.8937e-6, 6.9121e-6, 
            6.9005e-6, 6.9861e-6, 6.82e-6, 6.6089e-6, 6.5809e-6, 7.3496e-6, 
            8.0311e-6, 8.3186e-6, 8.426e-6, 9.0644e-6, 9.4965e-6, 9.4909e-6, 
            9.016e-6, 9.1494e-6, 9.3629e-6, 9.5944e-6, 9.5459e-6, 8.9919e-6, 
            8.604e-6, 7.8613e-6, 7.1567e-6, 6.2677e-6, 5.1899e-6, 4.4188e-6, 
            3.7167e-6, 3.0636e-6, 2.5573e-6, 2.0317e-6, 1.6371e-6, 1.3257e-6, 
            1.0928e-6, 8.9986e-7, 7.4653e-7, 6.1111e-7, 5.1395e-7, 4.35e-7, 
            3.7584e-7, 3.2633e-7, 2.8413e-7, 2.4723e-7, 2.1709e-7, 1.9294e-7, 
            1.7258e-7, 1.5492e-7, 1.382e-7, 1.2389e-7, 1.1189e-7, 1.0046e-7, 
            9.0832e-8, 8.2764e-8, 7.4191e-8, 6.7085e-8, 6.0708e-8, 5.4963e-8, 
            4.9851e-8, 4.5044e-8, 4.0916e-8, 3.722e-8, 3.3678e-8, 3.0663e-8, 
            2.7979e-8, 2.5495e-8, 2.3286e-8, 2.1233e-8, 1.9409e-8, 1.777e-8, 
            1.626e-8, 1.4885e-8, 1.3674e-8, 1.2543e-8, 1.1551e-8, 1.0655e-8, 
            9.8585e-9, 9.1398e-9, 8.4806e-9, 7.8899e-9, 7.3547e-9, 6.867e-9, 
            6.4131e-9, 5.993e-9, 5.6096e-9, 5.2592e-9, 4.9352e-9, 4.6354e-9, 
            4.3722e-9, 4.125e-9, 3.9081e-9, 3.7118e-9, 3.5372e-9, 3.3862e-9, 
            3.2499e-9, 3.1324e-9, 3.0313e-9, 2.9438e-9, 2.8686e-9, 2.805e-9, 
            2.7545e-9, 2.7149e-9, 2.6907e-9, 2.6724e-9, 2.6649e-9, 2.6642e-9, 
            2.6725e-9, 2.6871e-9, 2.7056e-9, 2.7357e-9, 2.7781e-9, 2.8358e-9, 
            2.9067e-9, 2.9952e-9, 3.102e-9, 3.2253e-9, 3.3647e-9, 3.5232e-9, 
            3.7037e-9, 3.9076e-9, 4.1385e-9, 4.3927e-9, 4.6861e-9, 5.0238e-9, 
            5.4027e-9, 5.8303e-9, 6.3208e-9, 6.8878e-9, 7.5419e-9, 8.313e-9, 
            9.1952e-9, 1.0228e-8, 1.1386e-8, 1.2792e-8, 1.4521e-8, 1.6437e-8, 
            1.8674e-8, 2.116e-8, 2.4506e-8, 2.8113e-8, 3.2636e-8, 3.7355e-8, 
            4.2234e-8, 4.9282e-8, 5.7358e-8, 6.6743e-8, 7.8821e-8, 9.4264e-8, 
            1.1542e-7, 1.3684e-7, 1.6337e-7, 2.0056e-7, 2.3252e-7, 2.6127e-7, 
            2.9211e-7, 3.3804e-7, 3.7397e-7, 3.8205e-7, 3.881e-7, 3.9499e-7, 
            3.9508e-7, 3.7652e-7, 3.5859e-7, 3.6198e-7, 3.7871e-7, 4.0925e-7, 
            4.2717e-7, 4.8241e-7, 5.2008e-7, 5.653e-7, 5.9531e-7, 6.1994e-7, 
            6.508e-7, 6.6355e-7, 6.9193e-7, 6.993e-7, 7.3058e-7, 7.4678e-7, 
            7.9193e-7, 8.3627e-7, 9.1267e-7, 1.0021e-6, 1.1218e-6, 1.2899e-6, 
            1.4447e-6, 1.7268e-6, 2.0025e-6, 2.3139e-6, 2.5599e-6, 2.892e-6, 
            3.3059e-6, 3.5425e-6, 3.9522e-6, 4.0551e-6, 4.2818e-6, 4.2892e-6, 
            4.421e-6, 4.5614e-6, 4.6739e-6, 4.9482e-6, 5.1118e-6, 5.0986e-6, 
            4.9417e-6, 4.9022e-6, 4.8449e-6, 4.8694e-6, 4.8111e-6, 4.9378e-6, 
            5.3231e-6, 5.7362e-6, 6.235e-6, 6.0951e-6, 5.7281e-6, 5.4585e-6, 
            4.9032e-6, 4.3009e-6, 3.4776e-6, 2.8108e-6, 2.2993e-6, 1.7999e-6, 
            1.387e-6, 1.075e-6, 8.5191e-7, 6.7951e-7, 5.5336e-7, 4.6439e-7, 
            4.0243e-7, 3.5368e-7, 3.1427e-7, 2.7775e-7, 2.4486e-7, 2.1788e-7, 
            1.9249e-7, 1.7162e-7, 1.5115e-7, 1.3478e-7, 1.2236e-7, 1.1139e-7, 
            1.0092e-7, 9.0795e-8, 8.2214e-8, 7.4691e-8, 6.7486e-8, 6.0414e-8, 
            5.4584e-8, 4.8754e-8, 4.3501e-8, 3.8767e-8, 3.4363e-8, 3.0703e-8, 
            2.7562e-8, 2.4831e-8, 2.2241e-8, 1.9939e-8, 1.8049e-8, 1.6368e-8, 
            1.4863e-8, 1.346e-8, 1.2212e-8, 1.1155e-8, 1.0185e-8, 9.3417e-9, 
            8.5671e-9, 7.8292e-9, 7.1749e-9, 6.5856e-9, 6.0588e-9, 5.5835e-9, 
            5.135e-9, 4.7395e-9, 4.3771e-9, 4.0476e-9, 3.756e-9, 3.4861e-9, 
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            8.7668e-11, 8.7951e-11, 9.2952e-11, 9.6157e-11, 9.5926e-11, 
            1.012e-10, 1.0115e-10, 9.9577e-11, 9.6633e-11, 9.2891e-11, 
            9.3315e-11, 9.5584e-11, 1.0064e-10, 1.0509e-10, 1.1455e-10, 
            1.2443e-10, 1.2963e-10, 1.2632e-10, 1.1308e-10, 1.0186e-10, 
            8.588e-11, 6.7863e-11, 5.1521e-11, 3.778e-11, 2.8842e-11, 
            2.2052e-11, 1.7402e-11, 1.4406e-11, 1.1934e-11, 1.0223e-11, 
            8.9544e-12, 7.9088e-12, 7.0675e-12, 6.2222e-12, 5.6051e-12, 
            5.0502e-12, 4.5578e-12, 4.2636e-12, 3.9461e-12, 3.7599e-12, 
            3.5215e-12, 3.2467e-12, 3.0018e-12, 2.6558e-12, 2.3928e-12, 
            2.0707e-12, 1.7575e-12, 1.5114e-12, 1.2941e-12, 1.1004e-12, 
            9.5175e-13, 8.2894e-13, 7.3253e-13, 6.5551e-13, 5.9098e-13, 
            5.3548e-13, 4.8697e-13, 4.4413e-13, 4.06e-13, 3.7188e-13, 
            3.4121e-13, 3.1356e-13, 2.8856e-13, 2.659e-13, 2.4533e-13, 
            2.2663e-13, 2.096e-13, 1.9407e-13, 1.799e-13, 1.6695e-13, 
            1.5512e-13, 1.4429e-13, 1.3437e-13, 1.2527e-13, 1.1693e-13, 
            1.0927e-13, 1.0224e-13, 9.5767e-14, 8.9816e-14, 8.4335e-14, 
            7.9285e-14, 7.4626e-14, 7.0325e-14, 6.6352e-14, 6.2676e-14, 
            5.9274e-14, 5.6121e-14, 5.3195e-14, 5.0479e-14, 4.7953e-14, 
            4.5602e-14, 4.3411e-14, 4.1367e-14, 3.9456e-14, 3.767e-14, 
            3.5996e-14, 3.4427e-14, 3.2952e-14, 3.1566e-14, 3.0261e-14, 
            2.903e-14, 2.7868e-14, 2.677e-14, 2.573e-14, 2.4745e-14, 
            2.3809e-14, 2.2921e-14, 2.2076e-14, 2.1271e-14, 2.0504e-14, 
            1.9772e-14, 1.9073e-14, 1.8404e-14, 1.7764e-14, 1.7151e-14, 
            1.6564e-14, 1.6e-14, 1.5459e-14, 1.4939e-14, 1.4439e-14, 
            1.3958e-14, 1.3495e-14, 1.3049e-14, 1.262e-14, 1.2206e-14, 
            1.1807e-14, 1.1422e-14, 1.105e-14, 1.0691e-14, 1.0345e-14, 
            1.001e-14, 9.687e-15, 9.3747e-15, 9.0727e-15, 8.7808e-15, 
            8.4986e-15, 8.2257e-15, 7.9617e-15, 7.7064e-15, 7.4594e-15, 
            7.2204e-15, 6.9891e-15, 6.7653e-15, 6.5488e-15, 6.3392e-15, 
            6.1363e-15, 5.9399e-15, 5.7499e-15, 5.5659e-15, 5.3878e-15, 
            5.2153e-15, 5.0484e-15, 4.8868e-15, 4.7303e-15, 4.5788e-15, 
            4.4322e-15, 4.2902e-15, 4.1527e-15, 4.0196e-15, 3.8907e-15, 
            3.7659e-15, 3.6451e-15, 3.5281e-15, 3.4149e-15, 3.3052e-15, 
            3.1991e-15, 3.0963e-15, 2.9967e-15, 2.9004e-15, 2.8071e-15, 
            2.7167e-15, 2.6293e-15, 2.5446e-15, 2.4626e-15, 2.3833e-15, 
            2.3064e-15, 2.232e-15, 2.16e-15, 2.0903e-15, 2.0228e-15, 
            1.9574e-15, 1.8942e-15, 1.8329e-15, 1.7736e-15, 1.7163e-15, 
            1.6607e-15, 1.6069e-15, 1.5548e-15, 1.5044e-15, 1.4557e-15, 
            1.4084e-15, 1.3627e-15, 1.3185e-15, 1.2757e-15, 1.2342e-15, 
            1.1941e-15, 1.1552e-15, 1.1177e-15, 1.0813e-15, 1.0461e-15, 
            1.012e-15, 9.79e-16, 9.4707e-16, 9.1618e-16, 8.8628e-16, 
            8.5734e-16, 8.2933e-16, 8.0223e-16, 7.76e-16, 7.5062e-16, 
            7.2606e-16, 7.0229e-16, 6.7929e-16, 6.5703e-16, 6.355e-16, 
            6.1466e-16, 5.9449e-16, 5.7498e-16, 5.561e-16, 5.3783e-16, 
            5.2015e-16, 5.0305e-16, 4.865e-16, 4.7049e-16, 4.55e-16, 
            4.4002e-16, 4.2552e-16, 4.1149e-16, 3.9792e-16, 3.8479e-16, 
            3.7209e-16, 3.5981e-16, 3.4792e-16, 3.3642e-16, 3.253e-16, 
            3.1454e-16, 3.0413e-16, 2.9406e-16, 2.8432e-16, 2.749e-16, 
            2.6579e-16, 2.5697e-16, 2.4845e-16, 2.402e-16, 2.3223e-16, 
            2.2451e-16, 2.1705e-16, 2.0984e-16, 2.0286e-16, 1.9611e-16, 
            1.8958e-16, 1.8327e-16, 1.7716e-16, 1.7126e-16, 1.6555e-16, 
            1.6003e-16, 1.5469e-16, 1.4952e-16, 1.4453e-16, 1.397e-16, 
            1.3503e-16 } };

struct s_sh2ob_ {
    double e_1[3];
    int e_2;
    } sh2ob_ = { {-20., 2e4, 10.}, 2003 };

struct s_s260a_ {
    double e_1[2003];
    } s260a_ = { {.1775, .17045, .16457, .17045, .1775, .20036, .21347, .22454,
             .23428, .23399, .23022, .20724, .19712, .18317, .16724, .1478, 
            .12757, .11626, .10098, .089033, .07977, .067416, .059588, 
            .051117, .046218, .042179, .034372, .029863, .025252, .022075, 
            .019209, .015816, .013932, .011943, .010079, .0087667, .0074094, 
            .0064967, .0055711, .0048444, .0042552, .0036953, .0032824, 
            .0029124, .0026102, .002337, .00211, .0019008, .0017145, .0015573,
             .0014206, .0012931, .0011803, .0010774, 9.8616e-4, 9.0496e-4, 
            8.3071e-4, 7.6319e-4, 7.0149e-4, 6.4637e-4, 5.9566e-4, 5.4987e-4, 
            5.0768e-4, 4.688e-4, 4.3317e-4, 4.0037e-4, 3.7064e-4, 3.4325e-4, 
            3.1809e-4, 2.9501e-4, 2.7382e-4, 2.543e-4, 2.363e-4, 2.1977e-4, 
            2.0452e-4, 1.9042e-4, 1.774e-4, 1.6544e-4, 1.5442e-4, 1.4425e-4, 
            1.3486e-4, 1.2618e-4, 1.1817e-4, 1.1076e-4, 1.0391e-4, 9.7563e-5, 
            9.1696e-5, 8.6272e-5, 8.1253e-5, 7.6607e-5, 7.2302e-5, 6.8311e-5, 
            6.4613e-5, 6.1183e-5, 5.8001e-5, 5.5048e-5, 5.2307e-5, 4.9761e-5, 
            4.7395e-5, 4.5197e-5, 4.3155e-5, 4.1256e-5, 3.9491e-5, 3.7849e-5, 
            3.6324e-5, 3.4908e-5, 3.3594e-5, 3.2374e-5, 3.1244e-5, 3.0201e-5, 
            2.924e-5, 2.8356e-5, 2.7547e-5, 2.6814e-5, 2.6147e-5, 2.5551e-5, 
            2.5029e-5, 2.4582e-5, 2.4203e-5, 2.3891e-5, 2.3663e-5, 2.3531e-5, 
            2.3483e-5, 2.3516e-5, 2.3694e-5, 2.4032e-5, 2.4579e-5, 2.5234e-5, 
            2.6032e-5, 2.7119e-5, 2.8631e-5, 3.0848e-5, 3.3262e-5, 3.6635e-5, 
            4.0732e-5, 4.5923e-5, 5.3373e-5, 6.1875e-5, 7.2031e-5, 8.598e-5, 
            9.8642e-5, 1.1469e-4, 1.3327e-4, 1.539e-4, 1.7513e-4, 2.0665e-4, 
            2.3609e-4, 2.622e-4, 2.8677e-4, 3.259e-4, 3.8624e-4, 4.157e-4, 
            4.5207e-4, 4.9336e-4, 5.45e-4, 5.8258e-4, 5.8086e-4, 5.6977e-4, 
            5.3085e-4, 4.802e-4, 4.3915e-4, 4.0343e-4, 3.7853e-4, 3.7025e-4, 
            3.9637e-4, 4.4675e-4, 4.7072e-4, 4.9022e-4, 5.2076e-4, 5.3676e-4, 
            5.2755e-4, 4.8244e-4, 4.5473e-4, 4.3952e-4, 3.9614e-4, 3.4086e-4, 
            2.9733e-4, 2.6367e-4, 2.3767e-4, 2.0427e-4, 1.7595e-4, 1.5493e-4, 
            1.3851e-4, 1.1874e-4, 1.0735e-4, 9.049e-5, 8.1149e-5, 7.4788e-5, 
            6.5438e-5, 5.8248e-5, 4.8076e-5, 4.3488e-5, 3.7856e-5, 3.3034e-5, 
            2.9592e-5, 2.6088e-5, 2.3497e-5, 2.0279e-5, 1.7526e-5, 1.5714e-5, 
            1.3553e-5, 1.2145e-5, 1.0802e-5, 9.7681e-6, 8.8196e-6, 7.8291e-6, 
            7.1335e-6, 6.4234e-6, 5.8391e-6, 5.3532e-6, 4.9079e-6, 4.5378e-6, 
            4.1716e-6, 3.8649e-6, 3.5893e-6, 3.3406e-6, 3.1199e-6, 2.9172e-6, 
            2.7348e-6, 2.5644e-6, 2.4086e-6, 2.2664e-6, 2.1359e-6, 2.0159e-6, 
            1.9051e-6, 1.8031e-6, 1.7074e-6, 1.6185e-6, 1.5356e-6, 1.4584e-6, 
            1.3861e-6, 1.3179e-6, 1.2545e-6, 1.1951e-6, 1.1395e-6, 1.0873e-6, 
            1.0384e-6, 9.925e-7, 9.4935e-7, 9.0873e-7, 8.705e-7, 8.3446e-7, 
            8.0046e-7, 7.6834e-7, 7.38e-7, 7.0931e-7, 6.8217e-7, 6.5648e-7, 
            6.3214e-7, 6.0909e-7, 5.8725e-7, 5.6655e-7, 5.4693e-7, 5.2835e-7, 
            5.1077e-7, 4.9416e-7, 4.7853e-7, 4.6381e-7, 4.5007e-7, 4.3728e-7, 
            4.255e-7, 4.145e-7, 4.0459e-7, 3.9532e-7, 3.8662e-7, 3.7855e-7, 
            3.7041e-7, 3.6254e-7, 3.542e-7, 3.4617e-7, 3.3838e-7, 3.3212e-7, 
            3.2655e-7, 3.1865e-7, 3.1203e-7, 3.067e-7, 3.0252e-7, 2.9749e-7, 
            2.9184e-7, 2.8795e-7, 2.8501e-7, 2.8202e-7, 2.7856e-7, 2.7509e-7, 
            2.7152e-7, 2.6844e-7, 2.6642e-7, 2.6548e-7, 2.6617e-7, 2.6916e-7, 
            2.7372e-7, 2.8094e-7, 2.9236e-7, 3.1035e-7, 3.2854e-7, 3.5481e-7, 
            3.9377e-7, 4.4692e-7, 5.0761e-7, 5.7715e-7, 6.7725e-7, 8.0668e-7, 
            9.3716e-7, 1.0797e-6, 1.1689e-6, 1.3217e-6, 1.4814e-6, 1.5627e-6, 
            1.6519e-6, 1.7601e-6, 1.906e-6, 2.0474e-6, 2.0716e-6, 2.0433e-6, 
            1.9752e-6, 1.8466e-6, 1.7526e-6, 1.6657e-6, 1.587e-6, 1.5633e-6, 
            1.652e-6, 1.8471e-6, 1.9953e-6, 2.0975e-6, 2.2016e-6, 2.2542e-6, 
            2.3081e-6, 2.3209e-6, 2.2998e-6, 2.3056e-6, 2.2757e-6, 2.2685e-6, 
            2.2779e-6, 2.2348e-6, 2.2445e-6, 2.3174e-6, 2.4284e-6, 2.529e-6, 
            2.734e-6, 2.972e-6, 3.2332e-6, 3.5392e-6, 3.9013e-6, 4.3334e-6, 
            4.9088e-6, 5.3428e-6, 5.9142e-6, 6.6106e-6, 7.4709e-6, 8.5019e-6, 
            9.6835e-6, 1.0984e-5, 1.2831e-5, 1.4664e-5, 1.708e-5, 2.0103e-5, 
            2.4148e-5, 2.7948e-5, 3.2855e-5, 3.9046e-5, 4.6429e-5, 5.6633e-5, 
            6.6305e-5, 7.6048e-5, 8.7398e-5, 1.0034e-4, 1.1169e-4, 1.2813e-4, 
            1.3354e-4, 1.3952e-4, 1.4204e-4, 1.4615e-4, 1.5144e-4, 1.5475e-4, 
            1.6561e-4, 1.7135e-4, 1.6831e-4, 1.6429e-4, 1.6353e-4, 1.6543e-4, 
            1.5944e-4, 1.5404e-4, 1.5458e-4, 1.6287e-4, 1.7277e-4, 1.8387e-4, 
            1.7622e-4, 1.636e-4, 1.5273e-4, 1.3667e-4, 1.2364e-4, 9.7576e-5, 
            7.914e-5, 6.4241e-5, 5.1826e-5, 4.1415e-5, 3.1347e-5, 2.5125e-5, 
            2.0027e-5, 1.6362e-5, 1.3364e-5, 1.1117e-5, 9.4992e-6, 8.1581e-6, 
            7.1512e-6, 6.2692e-6, 5.5285e-6, 4.9e-6, 4.3447e-6, 3.8906e-6, 
            3.4679e-6, 3.1089e-6, 2.8115e-6, 2.5496e-6, 2.2982e-6, 2.0861e-6, 
            1.8763e-6, 1.7035e-6, 1.5548e-6, 1.4107e-6, 1.2839e-6, 1.1706e-6, 
            1.0709e-6, 9.8099e-7, 8.9901e-7, 8.2394e-7, 7.5567e-7, 6.9434e-7, 
            6.3867e-7, 5.8845e-7, 5.4263e-7, 5.0033e-7, 4.6181e-7, 4.2652e-7, 
            3.9437e-7, 3.6497e-7, 3.3781e-7, 3.1292e-7, 2.9011e-7, 2.6915e-7, 
            2.4989e-7, 2.3215e-7, 2.1582e-7, 2.0081e-7, 1.87e-7, 1.7432e-7, 
            1.6264e-7, 1.5191e-7, 1.4207e-7, 1.3306e-7, 1.2484e-7, 1.1737e-7, 
            1.1056e-7, 1.0451e-7, 9.906e-8, 9.4135e-8, 8.9608e-8, 8.5697e-8, 
            8.1945e-8, 7.8308e-8, 7.4808e-8, 7.1686e-8, 6.8923e-8, 6.5869e-8, 
            6.3308e-8, 6.084e-8, 5.8676e-8, 5.6744e-8, 5.5016e-8, 5.3813e-8, 
            5.2792e-8, 5.2097e-8, 5.1737e-8, 5.1603e-8, 5.1656e-8, 5.1989e-8, 
            5.2467e-8, 5.2918e-8, 5.3589e-8, 5.456e-8, 5.5869e-8, 5.7403e-8, 
            5.8968e-8, 6.0973e-8, 6.3432e-8, 6.6245e-8, 6.9353e-8, 7.2686e-8, 
            7.6541e-8, 8.0991e-8, 8.595e-8, 9.1429e-8, 9.7851e-8, 1.0516e-7, 
            1.1349e-7, 1.2295e-7, 1.3335e-7, 1.4488e-7, 1.5864e-7, 1.7412e-7, 
            1.914e-7, 2.1078e-7, 2.3369e-7, 2.5996e-7, 2.8848e-7, 3.2169e-7, 
            3.5991e-7, 4.0566e-7, 4.5969e-7, 5.3094e-7, 6.1458e-7, 7.1155e-7, 
            8.3045e-7, 9.9021e-7, 1.2042e-6, 1.4914e-6, 1.8145e-6, 2.221e-6, 
            2.7831e-6, 3.4533e-6, 4.4446e-6, 5.1989e-6, 6.2289e-6, 7.1167e-6, 
            8.3949e-6, 9.6417e-6, 1.0313e-5, 1.0485e-5, 1.0641e-5, 1.0898e-5, 
            1.0763e-5, 1.0506e-5, 1.0497e-5, 1.1696e-5, 1.2654e-5, 1.3029e-5, 
            1.3175e-5, 1.4264e-5, 1.4985e-5, 1.4999e-5, 1.4317e-5, 1.4616e-5, 
            1.4963e-5, 1.5208e-5, 1.4942e-5, 1.3879e-5, 1.3087e-5, 1.1727e-5, 
            1.0515e-5, 9.0073e-6, 7.3133e-6, 6.1181e-6, 5.0623e-6, 4.1105e-6, 
            3.3915e-6, 2.6711e-6, 2.1464e-6, 1.7335e-6, 1.4302e-6, 1.1847e-6, 
            9.9434e-7, 8.2689e-7, 7.0589e-7, 6.075e-7, 5.3176e-7, 4.6936e-7, 
            4.1541e-7, 3.6625e-7, 3.2509e-7, 2.9156e-7, 2.6308e-7, 2.3819e-7, 
            2.1421e-7, 1.9366e-7, 1.7626e-7, 1.5982e-7, 1.4567e-7, 1.3354e-7, 
            1.2097e-7, 1.1029e-7, 1.0063e-7, 9.2003e-8, 8.4245e-8, 7.7004e-8, 
            7.0636e-8, 6.4923e-8, 5.9503e-8, 5.4742e-8, 5.045e-8, 4.647e-8, 
            4.2881e-8, 3.955e-8, 3.6541e-8, 3.3803e-8, 3.1279e-8, 2.8955e-8, 
            2.6858e-8, 2.4905e-8, 2.3146e-8, 2.1539e-8, 2.0079e-8, 1.8746e-8, 
            1.7517e-8, 1.6396e-8, 1.5369e-8, 1.4426e-8, 1.3543e-8, 1.2724e-8, 
            1.1965e-8, 1.1267e-8, 1.0617e-8, 1.001e-8, 9.4662e-9, 8.9553e-9, 
            8.4988e-9, 8.0807e-9, 7.7043e-9, 7.3721e-9, 7.0707e-9, 6.8047e-9, 
            6.5702e-9, 6.3634e-9, 6.1817e-9, 6.0239e-9, 5.8922e-9, 5.7824e-9, 
            5.7019e-9, 5.6368e-9, 5.594e-9, 5.5669e-9, 5.5583e-9, 5.5653e-9, 
            5.5837e-9, 5.6243e-9, 5.6883e-9, 5.78e-9, 5.8964e-9, 6.0429e-9, 
            6.2211e-9, 6.4282e-9, 6.6634e-9, 6.9306e-9, 7.2336e-9, 7.5739e-9, 
            7.9562e-9, 8.3779e-9, 8.8575e-9, 9.3992e-9, 1.0004e-8, 1.0684e-8, 
            1.145e-8, 1.232e-8, 1.3311e-8, 1.4455e-8, 1.5758e-8, 1.7254e-8, 
            1.8927e-8, 2.093e-8, 2.3348e-8, 2.6074e-8, 2.9221e-8, 3.277e-8, 
            3.7485e-8, 4.2569e-8, 4.8981e-8, 5.5606e-8, 6.2393e-8, 7.1901e-8, 
            8.2921e-8, 9.5513e-8, 1.1111e-7, 1.3143e-7, 1.5971e-7, 1.8927e-7, 
            2.2643e-7, 2.786e-7, 3.2591e-7, 3.7024e-7, 4.2059e-7, 4.9432e-7, 
            5.5543e-7, 5.7498e-7, 5.921e-7, 6.1005e-7, 6.1577e-7, 5.9193e-7, 
            5.6602e-7, 5.7403e-7, 6.005e-7, 6.4723e-7, 6.7073e-7, 7.5415e-7, 
            8.0982e-7, 8.7658e-7, 9.143e-7, 9.4459e-7, 9.8347e-7, 9.8768e-7, 
            1.0153e-6, 1.0066e-6, 1.0353e-6, 1.0353e-6, 1.0722e-6, 1.1138e-6, 
            1.1923e-6, 1.2947e-6, 1.4431e-6, 1.6537e-6, 1.8662e-6, 2.2473e-6, 
            2.6464e-6, 3.1041e-6, 3.4858e-6, 4.0167e-6, 4.6675e-6, 5.0983e-6, 
            5.7997e-6, 6.0503e-6, 6.4687e-6, 6.5396e-6, 6.7986e-6, 7.0244e-6, 
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            2.0127e-10, 2.3586e-10, 2.705e-10, 3.095e-10, 3.6584e-10, 
            4.1278e-10, 4.6591e-10, 5.222e-10, 5.5246e-10, 6.15e-10, 
            6.5878e-10, 7.1167e-10, 7.9372e-10, 8.6975e-10, 9.6459e-10, 
            9.7368e-10, 9.8142e-10, 1.0202e-9, 1.02e-9, 1.0356e-9, 1.0092e-9, 
            1.0269e-9, 1.0366e-9, 1.049e-9, 1.0717e-9, 1.0792e-9, 1.1016e-9, 
            1.0849e-9, 1.0929e-9, 1.0971e-9, 1.0969e-9, 1.046e-9, 9.2026e-10, 
            8.1113e-10, 6.8635e-10, 5.5369e-10, 4.2908e-10, 3.3384e-10, 
            2.648e-10, 2.081e-10, 1.6915e-10, 1.4051e-10, 1.1867e-10, 
            1.0158e-10, 8.899e-11, 7.9175e-11, 7.044e-11, 6.3453e-11, 
            5.7009e-11, 5.1662e-11, 4.7219e-11, 4.3454e-11, 4.0229e-11, 
            3.7689e-11, 3.6567e-11, 3.5865e-11, 3.5955e-11, 3.5928e-11, 
            3.6298e-11, 3.7629e-11, 3.93e-11, 4.1829e-11, 4.4806e-11, 
            5.0534e-11, 5.6672e-11, 6.2138e-11, 6.8678e-11, 7.6111e-11, 
            8.4591e-11, 9.2634e-11, 9.8085e-11, 1.083e-10, 1.1949e-10, 
            1.2511e-10, 1.3394e-10, 1.3505e-10, 1.4342e-10, 1.4874e-10, 
            1.492e-10, 1.5872e-10, 1.5972e-10, 1.5821e-10, 1.5425e-10, 
            1.4937e-10, 1.5089e-10, 1.5521e-10, 1.6325e-10, 1.6924e-10, 
            1.8265e-10, 1.9612e-10, 2.0176e-10, 1.9359e-10, 1.7085e-10, 
            1.5197e-10, 1.2646e-10, 9.8552e-11, 7.453e-11, 5.5052e-11, 
            4.2315e-11, 3.2736e-11, 2.6171e-11, 2.1909e-11, 1.8286e-11, 
            1.5752e-11, 1.3859e-11, 1.2288e-11, 1.1002e-11, 9.7534e-12, 
            8.8412e-12, 8.0169e-12, 7.2855e-12, 6.8734e-12, 6.4121e-12, 
            6.1471e-12, 5.778e-12, 5.3478e-12, 4.9652e-12, 4.4043e-12, 
            3.9862e-12, 3.4684e-12, 2.9681e-12, 2.5791e-12, 2.2339e-12, 
            1.9247e-12, 1.6849e-12, 1.4863e-12, 1.3291e-12, 1.2021e-12, 
            1.0947e-12, 1.0015e-12, 9.1935e-13, 8.4612e-13, 7.8036e-13, 
            7.21e-13, 6.6718e-13, 6.1821e-13, 5.7353e-13, 5.3269e-13, 
            4.9526e-13, 4.6093e-13, 4.2937e-13, 4.0034e-13, 3.7361e-13, 
            3.4895e-13, 3.2621e-13, 3.052e-13, 2.8578e-13, 2.6782e-13, 
            2.512e-13, 2.3581e-13, 2.2154e-13, 2.0832e-13, 1.9605e-13, 
            1.8466e-13, 1.7408e-13, 1.6425e-13, 1.5511e-13, 1.4661e-13, 
            1.3869e-13, 1.3131e-13, 1.2444e-13, 1.1803e-13, 1.1205e-13, 
            1.0646e-13, 1.0124e-13, 9.6358e-14, 9.1789e-14, 8.7509e-14, 
            8.3498e-14, 7.9735e-14, 7.6202e-14, 7.2882e-14, 6.976e-14, 
            6.6822e-14, 6.4053e-14, 6.1442e-14, 5.8978e-14, 5.665e-14, 
            5.4448e-14, 5.2364e-14, 5.0389e-14, 4.8516e-14, 4.6738e-14, 
            4.5048e-14, 4.3441e-14, 4.1911e-14, 4.0453e-14, 3.9063e-14, 
            3.7735e-14, 3.6467e-14, 3.5254e-14, 3.4093e-14, 3.298e-14, 
            3.1914e-14, 3.0891e-14, 2.9909e-14, 2.8965e-14, 2.8058e-14, 
            2.7185e-14, 2.6344e-14, 2.5535e-14, 2.4755e-14, 2.4002e-14, 
            2.3276e-14, 2.2576e-14, 2.1899e-14, 2.1245e-14, 2.0613e-14, 
            2.0002e-14, 1.9411e-14, 1.8839e-14, 1.8285e-14, 1.7749e-14, 
            1.723e-14, 1.6727e-14, 1.624e-14, 1.5768e-14, 1.531e-14, 
            1.4867e-14, 1.4436e-14, 1.4019e-14, 1.3614e-14, 1.3221e-14, 
            1.284e-14, 1.2471e-14, 1.2112e-14, 1.1764e-14, 1.1425e-14, 
            1.1097e-14, 1.0779e-14, 1.0469e-14, 1.0169e-14, 9.8775e-15, 
            9.5943e-15, 9.3193e-15, 9.0522e-15, 8.7928e-15, 8.5409e-15, 
            8.2962e-15, 8.0586e-15, 7.8278e-15, 7.6036e-15, 7.3858e-15, 
            7.1742e-15, 6.9687e-15, 6.7691e-15, 6.5752e-15, 6.3868e-15, 
            6.2038e-15, 6.026e-15, 5.8533e-15, 5.6856e-15, 5.5226e-15, 
            5.3642e-15, 5.2104e-15, 5.061e-15, 4.9158e-15, 4.7748e-15, 
            4.6378e-15, 4.5047e-15, 4.3753e-15, 4.2497e-15, 4.1277e-15, 
            4.0091e-15, 3.8939e-15, 3.782e-15, 3.6733e-15, 3.5677e-15, 
            3.4651e-15, 3.3655e-15, 3.2686e-15, 3.1746e-15, 3.0832e-15, 
            2.9944e-15, 2.9082e-15, 2.8244e-15, 2.7431e-15, 2.664e-15, 
            2.5872e-15, 2.5126e-15, 2.4401e-15, 2.3697e-15, 2.3014e-15, 
            2.2349e-15, 2.1704e-15, 2.1077e-15, 2.0468e-15, 1.9877e-15, 
            1.9302e-15, 1.8744e-15, 1.8202e-15, 1.7675e-15, 1.7164e-15, 
            1.6667e-15, 1.6184e-15, 1.5716e-15, 1.526e-15, 1.4818e-15, 
            1.4389e-15, 1.3971e-15, 1.3566e-15, 1.3172e-15, 1.279e-15, 
            1.2419e-15, 1.2058e-15, 1.1708e-15, 1.1368e-15, 1.1037e-15, 
            1.0716e-15, 1.0405e-15, 1.0102e-15, 9.8079e-16, 9.5224e-16, 
            9.2451e-16, 8.9758e-16, 8.7142e-16, 8.4602e-16, 8.2136e-16, 
            7.974e-16, 7.7414e-16, 7.5154e-16, 7.2961e-16, 7.083e-16, 
            6.8761e-16, 6.6752e-16, 6.4801e-16, 6.2906e-16, 6.1066e-16, 
            5.928e-16, 5.7545e-16, 5.586e-16, 5.4224e-16, 5.2636e-16, 
            5.1094e-16, 4.9596e-16} };

struct s_s260b_ {
    double e_1[3];
    int e_2;
    } s260b_ = { {-20., 2e4, 10.}, 2003 };

struct s_consts_ {
    double e_1[9];
    } consts_ = { {3.1415927410125732, 6.62606876e-27, 1.3806503e-16, 
            29979245800., 6.02214199e23, 2.6867775e19, 83144720., 
            1.191042722e-12, 1.4387752} };


/* Table of constant values */

/*
static integer c__9 = 9;
static integer c__1 = 1;
static integer c__2 = 2;
static integer c__5 = 5;
static int cs__0 = 0;
*/
// FIXME static double c_b125 = 0.;

/* ############################################################################ */
/*     path:            $Source: /srv/svn/cvs/cvsroot/arts/src/continua.cc,v $ */
/*     author:          $Author $ */
/*     revision:                $Revision: 1.26.2.21 $ */
/*     created:         $Date: 2005/06/09 11:01:30 $ */
/* ############################################################################ */

/* CKD2.4 TEST */
/* TKS, 2002-02-28 */
/* CALL : g77 -c testckd.f ; g77 testckd.o -o testckd */

/* ############################################################################ */
/* ----------------------------------------------------------------------------- */

/* INPUT PARAMETERS: */
/*  P          [hPa]  TOTAL PRESSURE */
/*  T          [K]    TEMPERATURE */
/*  VMRH2O     [1]    H2O VOLUME MIXING RATIO */
/*  VMRN2      [1]    N2  VOLUME MIXING RATIO */
/*  VMRO2      [1]    O2  VOLUME MIXING RATIO */
/*  FREQ       [Hz]   FREQUENCY OF ABSORPTION CALCULATION */


/* OUTPUT PARAMETER: */
/*  artsckd_     [1/m]  ABSORPTION COEFFICIENT */

/* ----------------------------------------------------------------------------- */

double artsckd_(double p, double t, double vmrh2o, 
        double vmrn2, double vmro2, double freq, int ivc)
{
    /* Initialized data */

    static double xslf = 1.;
    static double xfrg = 1.;
    static double xcn2 = 1.;

    /* System generated locals */
    double ret_val=0.0e0;
    // FIXME double d__1, d__2, d__3, d__4;

    /* Local variables */
    // FIXME int iosa;
    double w_wv__, oc_n2, radct;
    double w_other__, w_n2__, w_o2__;
    double of_wv, os_wv, p0, xn_wv__, t0, rhofac, wn, xn, xn0, tksvpt, rft;

    extern int initi_(double, double , double *, 
                      double *, double *, double *, double *, 
                      double *, double *, double *, double *, 
                      double *, double *);
    extern double fwv_(int , double , double *, double *, 
                       double *, double *, double *, double *);
    extern double swv_(int , double , double , double *, double *
                       , double *, double *, double *, double *, 
                       double *);
    extern double conti_n2__(double , double , double *, 
            double *, double *, double *, double *);


/*     PROGRAM:  MODM */
/*     ------- */

/*     AUTHOR: Sid-Ahmed Boukabara */
/*     ------ */

/*     AFFILIATION: ATMOSPHERIC AND ENVIRONMENTAL RESEARCH INC. */
/*     ----------- */

/*     DATE OF CREATION : October 1998 */
/*     ---------------- */

/*     AIM: This program is aimed at the calculation of the */
/*     ---  atmospheric optical depths. The spectral validity depends */
/*          only on the region covered by the file:"spectral_lines.dat" */
/*          The components treated here are the water vapor, the */
/*          oxygen, the ozone, the nitrogen and nitrogen dioxide. */

/*     - IVC      : Flag of contin. vers.: CKD2.4(if=2)  MPMf87/s93 (if=3) */
/*     - ICP      : Flag to take(if =1) or not (if=0) the line coupling */
/*     - NWN      : Number of wavenumbers to be treated */
/*     - WN       : Vector of NWN wavenumbers [in cm-1], one should note that */
/*                  this input could be a scalar (associated with NWN=1) */
/*     - NLAY     : Number of layers to be treated. */
/*     - P        : Vector of NLAY pressures (in mbar), one should note that */
/*                  this input could be a scalar (associated with NLAY=1) */
/*     - T        : Vector of NLAY temperatures [in Kelvin] */
/*     - W_WV     : Vector of NLAY water vapor column amounts [in molecules/cm2] */
/*     - W_O2     : Vector of NLAY oxygen column amounts [in molecules/cm2] */
/*     - W_N2     : Vector of NLAY nitrogen column amounts [in molecules/cm2] */
/*     - W_OTHER  : Vector of NLAY of other species column amounts [in molecules/cm2] */
/*     - CLW      : Vector of NLAY Cloud Liquid Water amounts [in kg/m2 or mm] */
/*                  When Cloud is present, the frequency must be consistent */
/*                  with Rayleigh absorption (no scattering performed in */
/*                  monortm). */
/*     - XSLF     : Scaling factor of the self WV continuum (usually XSLF=1) */
/*     - XFRG     : Scaling factor of the foreign WV continuum (usually XFRG=1) */
/*     - XCN2     : Scaling factor of the N2 continuum (usually XCN2=1) */
/*     - O        : An array of NWNxNLAY elts containing the total optical depths */
/*                  due to all the active species [in nepers] */
/*     - OS_WV    : An array of NWNxNLAY elts containing the water vapor optical */
/*                  depth (due to self continuum), [in Nepers] */
/*     - OF_WV    : An array of NWNxNLAY elts containing the water vapor optical */
/*                  depth (due to foreign continuum), [in Nepers] */
/*     - OC_N2    : An array of NWNxNLAY elts containing the nitrogen optical */
/*                  depth (due to continuum), [in Nepers] */
/*     - O_CLW    : An array of NWNxNLAY elts containing the CLW optical */
/*                  depth , [in Nepers] */

/*     History of the modifications: */
/*     ***************************** */
/*     - written in 1999 by Sid Ahmed Boukabara, Ross Hoffman */
/*      and Tony Clough. */
/*     - validated against ARM sondes in the */
/*      microwave spectrum (23.8 and 31.4 GHz). SAB, 2000. */
/*     - extended to more species by Sid Ahmed Boukabara in 03/2000. */
/*     - cleaned up and commented in 2001 for first public release. */
/*      Also put under CVS configuration management. SAB. */
/*     - Extended O2 lines to submillimeter. Extensive validation */
/*      by comparison to Rosenkranz model and MWR data. */
/*      Update of the LBLATM module (accepts inputs at pressure */
/*      grid, along with altitude grid). */
/*      Fixed the handling of N2 amount coming from LBLATM (which */
/*      depends on the number of molecules NMOL). */
/*      Adopted accurate constants values. */
/*      Sid Ahmed Boukabara. Dec 14th 2001. */
/*     - Updated on January 7th 2002. ARM option (INP=2) updated and */
/*       made more efficient after Jim's comments. (INP=3) option optimized. */
/*       WV line intensities modified in the microwave (see Tony's email). */

/*     Comments should be forwarded to Sid Ahmed Boukabara (sboukaba@aer.com) */
/*     or Tony Clough (clough@aer.com). */

/* ============================================================================ */


/* TKS functions: */

/*     scaling factor (SLF cont) */
/*     scaling factor (FRG cont) */
/*     scaling factor (N2 cont) */


    w_wv__ = 0.0e0;
    w_o2__ = 0.0e0;
    w_n2__ = 0.0e0;
    w_other__ = 0.0e0;
    ret_val = 0.0e0;
    rft = 0.0e0;
    os_wv = 0.0e0;
    of_wv = 0.0e0;
    oc_n2 = 0.0e0;

/*      ---INPUTS & GENERAL CONTROL PARAMETERS */

    /*     set H2O, O2 and N2 number density to column amount [molec/cm2] */
    /*     TKSVPT = P[Pa] / T[K] */
    tksvpt    = (p * 100.0) / t;
    /*     7.242923e16 = k_B [J/K] * 1.0e-6 [m^3/cm^3] */
    w_wv__    = vmrh2o * 7.242923e16 * tksvpt;
    w_o2__    = vmro2  * 7.242923e16 * tksvpt;
    w_n2__    = vmrn2  * 7.242923e16 * tksvpt;
    w_other__ = (1.0000E0-vmrh2o-vmro2-vmrn2) * 7.242923e16 * tksvpt; 

      /*     frequency [Hz] to wave number [cm-1] */
    wn = freq / 29979245800.0;
    //cout << "CKD2.4 H2O column amounts    [molec/cm2] =" << w_wv__ << "\n";
    //cout << "CKD2.4 O2 column amounts     [molec/cm2] =" << w_o2__ << "\n";
    //cout << "CKD2.4 H2O column amounts    [molec/cm2] =" << w_n2__ << "\n";
    //cout << "CKD2.4 others column amounts [molec/cm2] =" << w_other__ << "\n";
    //cout << "freq=" << freq << " Hz,   wave num=" << wn << " cm-1\n";

/* ---------------------------------------------------------------------------- */

/*     --- INITIALIZATION ----------------------------------------- */
    initi_(p, t, &radct, &t0, &p0, &w_wv__, &w_o2__, &w_n2__, &w_other__, &
            xn0, &xn, &xn_wv__, &rhofac);
    //cout << "CKD2.4 t0=" << t0 << "  p0=" << p0 << "\n";
    //cout << "radct   =" << radct << "\n";
    //cout << "xn0     =" << xn0 << "\n";
    //cout << "xn      =" << xn << "\n";
    //cout << "xn_wv__ =" << xn_wv__ << "\n";
    //cout << "rhofac  =" << rhofac << "\n";

    /*     --- RAD_FIELD_TERM ----------------------------------------- */
    rft = wn * tanh(radct * wn / (t * 2));
    //cout << "rft =" << rft << "\n";

    /*     --- H2O CONTINUUM TERM ------------------------------------- */

    if (ivc == 21) {
      /* CKD2.4  CONT_SELF_WV [Np/m] */
        os_wv = 1.0000e2 * swv_(2, wn, t, &t0, &w_wv__, &rft, &xn, &xn_wv__, &xn0, &xslf);
        //cout << "CKD2.4 ivc=21, H2O self cont  [in Np/m]   =" << os_wv << "\n";
        return os_wv;
    }
    if (ivc == 31) {
      /* MPMf87/s93  CONT_SELF_WV [Np/m] */
        os_wv = 1.0000e2 * swv_(3, wn, t, &t0, &w_wv__, &rft, &xn, &xn_wv__, &xn0, &xslf);
        //cout << "CKD2.4 ivc=31, H2O self cont  [in Np/m]   =" << os_wv << "\n";
        return os_wv;
    }
    if (ivc == 22) {
      /* CKD2.4  CONT_FRGN_WV [Np/m] */
        of_wv = 1.0000e2 * fwv_(2, wn, &w_wv__, &rft, &xn, &xn_wv__, &xn0, &xfrg);
        //cout << "CKD2.4 ivc=22, H2O foreign cont [in Np/m] =" << of_wv << "\n";
        return of_wv;
      }
    if (ivc == 32) {
      /* MPMf87/s93  CONT_FRGN_WV [Np/m] */
        of_wv = 1.0000e2 * fwv_(3, wn, &w_wv__, &rft, &xn, &xn_wv__, &xn0, &xfrg);
        //cout << "CKD2.4 ivc=32, H2O foreign cont [in Np/m] =" << of_wv << "\n";
        return of_wv ;
    }

    /* --- N2 CONTINUUM TERM [Np/m] ----------------------------------- */
    if (ivc == 1) {
        oc_n2 = 1.0000e2 * conti_n2__(wn, t, &t0, &w_n2__, &rft, &rhofac, &xcn2);
        //cout << "CKD2.4 ivc=1, N2 cont           [in Np/m] =" << oc_n2 << "\n";
        return oc_n2;
    }

    /* --- TOTAL ABSORPTION IN [in Np/m] --------------------------- */
    //    cout << "CKD2.4 H2O s+f cont         [in Np/m]         =" << ((os_wv+of_wv) * 1.0000e2) << "\n";
    //ret_val = ((os_wv + of_wv + oc_n2) * 1.0000e2);

// FIXME L999:

    return ret_val;  // [Np/m] 
} /* artsckd_ */


/* ############################################################################ */
/*     foreign continuum functions -------------------------------------------- */
double fwv_(int ivc, double wn, double *w_wv__, double *rft, 
            double *xn, double *xn_wv__, double *xn0, double *xfrg)
{
    /* System generated locals */
    double ret_val = 0.0e0;

    /* Local variables */
    extern double fwv24_(double , double *, double *, 
            double *, double *, double *, double *), 
            fwv_mpmf87s93__(double , double *, double *, 
            double *, double *, double *, double *);

    ret_val = 0.0e0;

/*     --- CKD2.4 CONTINUUM ------------------------------------- */
    if (ivc == 2 && *w_wv__ > 0.) {
        ret_val = fwv24_(wn, w_wv__, rft, xn, xn_wv__, xn0, xfrg);
    }


/*     --- MPMf87s93 CONTINUUM ---------------------------------- */
    if (ivc == 3 && *w_wv__ > 0.) {
        ret_val = fwv_mpmf87s93__(wn, w_wv__, rft, xn, xn_wv__, xn0, xfrg);
    }

    return ret_val;
} /* fwv_ */

double fwv_mpmf87s93__(double wn, double *w_wv__, double *rft, 
                       double *xn, double *xn_wv__, double *xn0, double *xfrg)
{
    /* System generated locals */
    double ret_val=0.0e0;

    /* Local variables */
    extern double xlgr_(double *, double *);
    int i__, j;
    double x[4], fscal, xf;

    ret_val = 0.0e0;

    j = (int) ((wn - fh2ob_1.v1) / fh2ob_1.dv) + 1;

    for (i__ = 1; i__ <= 4; ++i__) {
        x[i__ - 1] = fh2oa_1.fh2o[j + i__ - 3];
    }

    xf = (wn - (fh2ob_1.v1 + fh2ob_1.dv * (double) (j - 1))) / 
            fh2ob_1.dv;
    fscal = .8;
    ret_val = xlgr_(&xf, x) * 1e-20 * (*w_wv__ * *rft * ((*xn - *xn_wv__) / *
            xn0)) * fscal * *xfrg;

/* L999: */
    return ret_val;
} /* fwv_mpmf87s93__ */

double fwv24_(double wn, double *w_wv__, double *rft, 
              double *xn, double *xn_wv__, double *xn0, double *
              xfrg)
{
    /* Initialized data */

  static double v0f1 = 350.;
  static double hwsqf1 = 4e4;
  static double betaf1 = 5e-9;
  static double factrf1 = -.7;
  static double v0f1a = 630.;
  static double hwsqf1a = 4225.;
  static double betaf1a = 2e-8;
  static double factrf1a = .75;
  static double v0f2 = 1130.;
  static double hwsqf2 = 108900.;
  static double betaf2 = 8e-11;
  static double factrf2 = -.97;
  static double v0f3 = 1975.;
  static double hwsqf3 = 62500.;
  static double betaf3 = 5e-6;
  static double factrf3 = -.65;
  
  /* System generated locals */
  double ret_val=0.0e0;
  double d__1;
  
  /* Local variables */
  extern double xlgr_(double *, double *);
  int i__, j;
  double x[4], fscal, xf, vf2, vf4, vf6;

  ret_val = 0.0e0;
  
  j = (int) ((wn - fh2ob_1.v1) / fh2ob_1.dv) + 1;
  for (i__ = 1; i__ <= 4; ++i__) {
    x[i__ - 1] = fh2oa_1.fh2o[j + i__ - 3];
  }

  xf = (wn - (fh2ob_1.v1 + fh2ob_1.dv * (double) (j - 1))) / 
        fh2ob_1.dv;

/*     ---added correction to the forgn continuum */
/* Computing 2nd power */
    d__1  = wn - v0f1;
    vf2   = d__1 * d__1;
    vf6   = vf2 * vf2 * vf2;
    fscal = factrf1 * (hwsqf1 / (vf2 + betaf1 * vf6 + hwsqf1)) + 1.;
/* Computing 2nd power */
    d__1   = wn - v0f1a;
    vf2    = d__1 * d__1;
    vf6    = vf2 * vf2 * vf2;
    fscal *= factrf1a * (hwsqf1a / (vf2 + betaf1a * vf6 + hwsqf1a)) + 1.;
/* Computing 2nd power */
    d__1 = wn - v0f2;
    vf2 = d__1 * d__1;
    vf6 = vf2 * vf2 * vf2;
    fscal *= factrf2 * (hwsqf2 / (vf2 + betaf2 * vf6 + hwsqf2)) + 1.;
/* Computing 2nd power */
    d__1 = wn - v0f3;
    vf2 = d__1 * d__1;
    vf4 = vf2 * vf2;
    fscal *= factrf3 * (hwsqf3 / (vf2 + betaf3 * vf4 + hwsqf3)) + 1.;
    ret_val = xlgr_(&xf, x) * 1e-20 * (*w_wv__ * *rft * ((*xn - *xn_wv__) / *
            xn0)) * fscal * *xfrg;

/* L999: */
    return ret_val;
} /* fwv24_ */



/*     self continuum function ------------------------------------------------ */
double swv_(int ivc, double wn, double t, double *t0, 
            double *w_wv__, double *rft, double *xn, double *
            xn_wv__, double *xn0, double *xslf)
{
  /* System generated locals */
  double ret_val;

    /* Local variables */
    extern double swv_mpmf87s93__(double , double , double *
                                  , double *, double *, double *, double *, 
                                  double *, double *); 
    extern double swv24_(double , double , 
                         double *, double *, double *, double *, 
                         double *, double *, double *);
    
    ret_val = 0.;

/*     CKD2.4 CONTINUUM */
    if (ivc == 2 && *w_wv__ > 0.) {
/*     CNT_SLF_WV CKD2.4 */
        ret_val = swv24_(wn, t, t0, w_wv__, rft, xn, xn_wv__, xn0, xslf);
    }

    if (ivc == 3 && *w_wv__ > 0.) {
/*     MPMf87s93 CKD2.4 CONT. */
/*     CNT_SLF_WV */
        ret_val = swv_mpmf87s93__(wn, t, t0, w_wv__, rft, xn, xn_wv__, xn0, 
                xslf);
    }

    return ret_val;
} /* swv_ */



double swv24_(double wn, double t, double *t0, double *
              w_wv__, double *rft, double * /* xn */, double *xn_wv__, 
              double *xn0, double *xslf)
{
    /* Initialized data */

  static double v0s1 = 0.;
  static double hwsq1 = 1e4;
  static double betas1 = 1e-4;
  static double factrs1 = .688;
  static double v0s2 = 1050.;
  static double hwsq2 = 4e4;
  static double factrs2 = -.2333;
  static double v0s3 = 1310.;
  static double hwsq3 = 14400.;
  static double betas3 = 5e-6;
  static double factrs3 = -.15;

    /* System generated locals */
    double ret_val, d__1, d__2;

    /* Local variables */
    double sfac;
    extern double xlgr_(double *, double *);
    int j;
    double x[4], xf, vs2, vs4;

/*     ---UNITS(CM**3/MOL)*1.E-20 */

    ret_val = 0.;

    j = (int) ((wn - sh2ob_1.v1) / sh2ob_1.dv) + 1;
    d__1 = s260a_1.swv260[j - 2] / sh2oa_1.swv296[j - 2];
    d__2 = (t - *t0) / (260. - *t0);
    x[0] = sh2oa_1.swv296[j - 2] * pow(d__1, d__2);
    d__1 = s260a_1.swv260[j - 1] / sh2oa_1.swv296[j - 1];
    d__2 = (t - *t0) / (260. - *t0);
    x[1] = sh2oa_1.swv296[j - 1] * pow(d__1, d__2);
    d__1 = s260a_1.swv260[j] / sh2oa_1.swv296[j];
    d__2 = (t - *t0) / (260. - *t0);
    x[2] = sh2oa_1.swv296[j] * pow(d__1, d__2);
    d__1 = s260a_1.swv260[j + 1] / sh2oa_1.swv296[j + 1];
    d__2 = (t - *t0) / (260. - *t0);
    x[3] = sh2oa_1.swv296[j + 1] * pow(d__1, d__2);
    xf = (wn - (sh2ob_1.v1 + sh2ob_1.dv * (double) (j - 1))) / 
            sh2ob_1.dv;
    sfac = 1.;
/* Computing 2nd power */
    d__1 = wn - v0s1;
    vs2 = d__1 * d__1;
    vs4 = vs2 * vs2;
/* Computing 2nd power */
    d__1 = wn;
    sfac *= factrs1 * (hwsq1 / (d__1 * d__1 + betas1 * vs4 + hwsq1)) + 1.;
/* Computing 2nd power */
    d__1 = wn - v0s2;
    vs2 = d__1 * d__1;
    sfac *= factrs2 * (hwsq2 / (vs2 + hwsq2)) + 1.;
/* Computing 2nd power */
    d__1 = wn - v0s3;
    vs2 = d__1 * d__1;
    vs4 = vs2 * vs2;
    sfac *= factrs3 * (hwsq3 / (vs2 + betas3 * vs4 + hwsq3)) + 1.;
    ret_val = *w_wv__ * *rft * (*xn_wv__ / *xn0) * xlgr_(&xf, x) * 1e-20 * 
            sfac * *xslf;

    return ret_val;
} /* swv24_ */

double swv_mpmf87s93__(double wn, double t, double *t0, 
        double *w_wv__, double *rft, double * /* xn */, double *
        xn_wv__, double *xn0, double *xslf)
{
    /* System generated locals */
    double ret_val, d__1, d__2;

    /* Local variables */
    double sfac;
    extern double xlgr_(double *, double *);
    int j;
    double x[4], xf;

/*     ---UNITS(CM**3/MOL)*1.E-20 */

    ret_val = 0.;

    j = (int) ((wn - sh2ob_1.v1) / sh2ob_1.dv) + 1;
    d__1 = s260a_1.swv260[j - 2] / sh2oa_1.swv296[j - 2];
    d__2 = (t - *t0) / (260. - *t0);
    x[0] = sh2oa_1.swv296[j - 2] * pow(d__1, d__2);
    d__1 = s260a_1.swv260[j - 1] / sh2oa_1.swv296[j - 1];
    d__2 = (t - *t0) / (260. - *t0);
    x[1] = sh2oa_1.swv296[j - 1] * pow(d__1, d__2);
    d__1 = s260a_1.swv260[j] / sh2oa_1.swv296[j];
    d__2 = (t - *t0) / (260. - *t0);
    x[2] = sh2oa_1.swv296[j] * pow(d__1, d__2);
    d__1 = s260a_1.swv260[j + 1] / sh2oa_1.swv296[j + 1];
    d__2 = (t - *t0) / (260. - *t0);
    x[3] = sh2oa_1.swv296[j + 1] * pow(d__1, d__2);
    xf = (wn - (sh2ob_1.v1 + sh2ob_1.dv * (double) (j - 1))) / 
            sh2ob_1.dv;
    sfac = 3.;
    ret_val = *w_wv__ * *rft * (*xn_wv__ / *xn0) * xlgr_(&xf, x) * 1e-20 * 
            sfac * *xslf;

/* L999: */
    return ret_val;
} /* swv_mpmf87s93__ */

/*     --- N2 continuum ------------------------------------------------------- */
double conti_n2__(double wn, double t, double *t0, 
        double *w_n2__, double *rft, double *rhofac, double *
        xcn2)
{
    /* Initialized data */

    static double v1 = -10.;
    static double dv = 5.;
    static double ct296[73] = { 4.303e-7,4.85e-7,4.979e-7,4.85e-7,
            4.303e-7,3.715e-7,3.292e-7,3.086e-7,2.92e-7,2.813e-7,2.804e-7,
            2.738e-7,2.726e-7,2.724e-7,2.635e-7,2.621e-7,2.547e-7,2.428e-7,
            2.371e-7,2.228e-7,2.1e-7,1.991e-7,1.822e-7,1.697e-7,1.555e-7,
            1.398e-7,1.281e-7,1.138e-7,1.012e-7,9.078e-8,7.879e-8,6.944e-8,
            6.084e-8,5.207e-8,4.54e-8,3.897e-8,3.313e-8,2.852e-8,2.413e-8,
            2.045e-8,1.737e-8,1.458e-8,1.231e-8,1.031e-8,8.586e-9,7.162e-9,
            5.963e-9,4.999e-9,4.226e-9,3.607e-9,3.09e-9,2.669e-9,2.325e-9,
            2.024e-9,1.783e-9,1.574e-9,1.387e-9,1.236e-9,1.098e-9,9.777e-10,
            8.765e-10,7.833e-10,7.022e-10,6.317e-10,5.65e-10,5.1e-10,
            4.572e-10,4.115e-10,3.721e-10,3.339e-10,3.005e-10,2.715e-10,
            2.428e-10 };
    static double ct220[73] = { 4.946e-7,5.756e-7,5.964e-7,5.756e-7,
            4.946e-7,4.145e-7,3.641e-7,3.482e-7,3.34e-7,3.252e-7,3.299e-7,
            3.206e-7,3.184e-7,3.167e-7,2.994e-7,2.943e-7,2.794e-7,2.582e-7,
            2.468e-7,2.237e-7,2.038e-7,1.873e-7,1.641e-7,1.474e-7,1.297e-7,
            1.114e-7,9.813e-8,8.309e-8,7.059e-8,6.068e-8,5.008e-8,4.221e-8,
            3.537e-8,2.885e-8,2.407e-8,1.977e-8,1.605e-8,1.313e-8,1.057e-8,
            8.482e-9,6.844e-9,5.595e-9,4.616e-9,3.854e-9,3.257e-9,2.757e-9,
            2.372e-9,2.039e-9,1.767e-9,1.548e-9,1.346e-9,1.181e-9,1.043e-9,
            9.11e-10,8.103e-10,7.189e-10,6.314e-10,5.635e-10,4.976e-10,
            4.401e-10,3.926e-10,3.477e-10,3.085e-10,2.745e-10,2.416e-10,
            2.155e-10,1.895e-10,1.678e-10,1.493e-10,1.31e-10,1.154e-10,
            1.019e-10,8.855e-11 };

    /* System generated locals */
    double ret_val, d__1, d__2;

    /* Local variables */
    extern double xlgr_(double *, double *);
    int j;
    double x[4], xf;

/* TKS      INTEGER NPTCONTN2 */
/* TKS      INTEGER NPTCONTN2B */
/* TKS     &                 V1B,V2B,DVB */
/* TKS      DATA V2        / 350.0 / */
/* TKS      DATA NPTCONTN2 / 73    / */
/* TKS      DATA V1B, V2B, DVB, NPTCONTN2B / -10., 350., 5.0, 73 / */



    ret_val = 0.;
/* TKS  -- begin implementation of TKS */
    if (wn <= 0.) {
        ret_val = 0.;
        return ret_val;
    }
    if (wn > 350.) {
        ret_val = 0.;
        return ret_val;
    }
/* TKS  -- end implementation of TKS */

    if (*w_n2__ == 0.) {
        ret_val = 0.;
        return ret_val;
    }

    j = (int) ((wn - v1) / dv) + 1;
    d__1 = ct296[j - 2] / ct220[j - 2];
    d__2 = (t - *t0) / (220. - *t0);
    x[0] = ct296[j - 2] * pow(d__1, d__2);
    d__1 = ct296[j - 1] / ct220[j - 1];
    d__2 = (t - *t0) / (220. - *t0);
    x[1] = ct296[j - 1] * pow(d__1, d__2);
    d__1 = ct296[j] / ct220[j];
    d__2 = (t - *t0) / (220. - *t0);
    x[2] = ct296[j] * pow(d__1, d__2);
    d__1 = ct296[j + 1] / ct220[j + 1];
    d__2 = (t - *t0) / (220. - *t0);
    x[3] = ct296[j + 1] * pow(d__1, d__2);
    xf = (wn - (v1 + dv * (double) (j - 1))) / dv;
    ret_val = xlgr_(&xf, x) * 1e-20 * (*w_n2__ / .26867775 * *rft * *rhofac) *
             *xcn2;

    return ret_val;
} /* conti_n2__ */

/*     --- 4 points Lagrange interpolation ----------------------------------- */
double xlgr_(double *xf, double *x)
{
    /* System generated locals */
    double ret_val;

    /* Local variables */
    double a[4], b;




/*     with continous derivatives */
    /* Parameter adjustments */
    --x;

    /* Function Body */
    b = *xf * .5 * (1. - *xf);
    a[0] = -b * (1. - *xf);
    a[1] = 1. - (3. - *xf * 2.) * *xf * *xf + b * *xf;
    a[2] = (3. - *xf * 2.) * *xf * *xf + b * (1. - *xf);
    a[3] = -(b * *xf);
    ret_val = a[0] * x[1] + a[1] * x[2] + a[2] * x[3] + a[3] * x[4];

/* L999: */
    return ret_val;
} /* xlgr_ */

/*     --- initializations ---------------------------------------------------- */
int initi_(double p, double t, double *radct, 
        double *t0, double *p0, double *w_wv__, double *
        w_o2__, double *w_n2__, double *w_other__, double *xn0, 
        double *xn, double *xn_wv__, double *rhofac)
{
    /* Initialized data */

    static double wvmolmass = 18.016;
    static double drymolmass = 28.97;

    double wdry, ratiomix, wvpress;

/*     [K] */
    *t0 = 296.;
/*     [hPa] */
    *p0 = 1013.25;

/*     [K/cm-1] */
    *radct   = consts_1.planck * consts_1.clight / consts_1.boltz;
    *xn0     = *p0 / (consts_1.boltz * *t0) * 1e3;
    *xn      = p / (consts_1.boltz * t) * 1e3;
    wdry     = *w_o2__ + *w_n2__ + *w_other__;
    ratiomix = *w_wv__ * wvmolmass / (wdry * drymolmass);
    wvpress  = ratiomix / (ratiomix + wvmolmass / drymolmass) * p;
    *xn_wv__ = wvpress / (consts_1.boltz * t) * 1e3;
    *rhofac  = *w_n2__ / (wdry + *w_wv__) * (p / *p0) * (273.15 / t);

/* L999: */
    return 0;
} /* initi_ */

/* ############################################################################ */
/* ---Block data to be consistent with LBLRTM/LBLATM */
/* Subroutine */ int phys_consts__(void)
{
    return 0;
} /* phys_consts__ */


/*     Pi was obtained from PI = 2.*ASIN(1.) */
/* --------------------------------------------- */
/*       Constants from NIST 01/11/2002 */
/* --------------------------------------------- */
/* --------------------------------------------- */
/*       units are generally cgs */
/*       The first and second radiation constants are taken from NIST. */
/*       They were previously obtained from the relations: */
/*       RADCN1 = 2.*PLANCK*CLIGHT*CLIGHT*1.E-07 */
/*       RADCN2 = PLANCK*CLIGHT/BOLTZ */
/* --------------------------------------------- */

/* ############################################################################ */
/* Subroutine */ int bsa296_(void)
{
    return 0;
} /* bsa296_ */







/* Subroutine */ int bsb296_(void)
{
    return 0;
} /* bsb296_ */







/* ---------------------------------------------------------------------------- */


/* Subroutine */ int bs260a_(void)
{
    return 0;
} /* bs260a_ */








/* Subroutine */ int bs260b_(void)
{
    return 0;
} /* bs260b_ */







/* ---------------------------------------------------------------------------- */


/* Subroutine */ int bfh2oa_(void)
{
    return 0;
} /* bfh2oa_ */








/* Subroutine */ int bfh2ob_(void)
{
    return 0;
} /* bfh2ob_ */


// ---------------------- end of monortm CKD F77  code --------------------------

---