continua.h File Reference

This header file contains all the declarations of the implemented continua and full absorption (lines+continuum) models. More...

#include "matpackI.h"
#include "mystring.h"

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Detailed Description

This header file contains all the declarations of the implemented continua and full absorption (lines+continuum) models.

This is the file from arts-1-0, back-ported to arts-1-1.

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition in file continua.h.

Function Documentation

void BF86_CIA_N2	(	MatrixView	pxsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

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

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of N2-CIA according to BF-86 model [1/m]
	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_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	N2 volume mixing ratio profile [1]

Note:: this "crude" version of the N2-N2 model is a f2c conversion of the N2-N2 F77 code of Prof. A. Borysow. The original code can be downloaded at F77 code.

Remarks:: Reference: A. Borysow and L. Frommhold, The Astrophysical Journal, vol.311, pp.1043-1057, 1986 see for a scanned version of the paper.

Author:: Thomas Kuhn

Date:: 2002-03-05

Definition at line 7752 of file continua.cc.

References n2n2tks_(), ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), and out3.

Referenced by xsec_continuum_tag().

void check_continuum_model ( const String & name )

An auxiliary functions that checks if a given continuum model is listed in species_data.cc.

This is just in order to verify that this really represent a valid continuum model.

The given name should be something like `ContStandardSelf'. The function simply checks if there is a species H2O with an isotope ContStandardSelf.

For user-friendliness, the function also compiles a list of allowed continuum models and gives this as an error message if the model is not found.

The function has no return value, since, if the name does not match a valid model an error is thrown anyway.

Parameters:

name

The name of the continuum model to check.

Exceptions:

runtime_error

The model does not exist.

Author:: Stefan Buehler

Date:: 2001-03-12

Definition at line 12663 of file continua.cc.

References species_data.

Referenced by abs_cont_descriptionAppend(), and abs_xsec_per_speciesAddConts().

void CKD24_H20	(	MatrixView	pxsec,
		int	isf,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr,
		ConstVectorView	abs_n2
	)

CKD version 2.4 H2O continuum absorption model.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of H2O continuum according to CKD2.4 [1/m]
	isf	=0 self continuum, =1 foreign continuum
	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_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	H2O volume mixing ratio profile [1]
	abs_n2	N2 volume mixing ratio profile [1]

Note:: this "crude" version of the CKD2.4 model is a f2c conversion of the F77 code taken out of MonoRTM RT-model written by
S. BOUKABARA, S.A. CLOUGH, and R. HOFFMAN
Atmospheric and Environmental Research Inc. (AER),
Radiation and Climate Group
131 Hartwell Avenue
Lexington, MA 02421
USA
E-mail: sboukaba@aer.com, clough@aer.com

Remarks:: Reference: A. Borysow and L. Frommhold, The Astrophysical Journal, vol.311, pp.1043-1057, 1986 see for a scanned version of the paper.

Author:: Thomas Kuhn

Date:: 2002-03-06

Definition at line 5128 of file continua.cc.

References artsckd_(), ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), and out3.

Referenced by xsec_continuum_tag().

void CKD_222_foreign_h2o	(	MatrixView	pxsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr,
		ConstVectorView	abs_n2
	)

CKD version 2.2.2 H2O foreign continuum absorption model.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of H2O foreign continuum according to CKDv.2.2.2 [1/m]
	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_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	H2O volume mixing ratio profile [1]
	abs_n2	N2 volume mixing ratio profile [1]

Note:: This absorption model is taken from the FORTRAN77 code of CKD version 2.2.2 written by
Atmospheric and Environmental Research Inc. (AER),
Radiation and Climate Group
131 Hartwell Avenue
Lexington, MA 02421, USA
http://www.rtweb.aer.com/continuum_frame.html

Author:: Thomas Kuhn

Date:: 2002-28-08

Definition at line 2385 of file continua.cc.

References addF77fields, FH2O_ckd_0, FH2O_ckd_0_dv, FH2O_ckd_0_npt, FH2O_ckd_0_v1, FH2O_ckd_0_v2, ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, RADFN_FUN(), SPEED_OF_LIGHT, and XINT_FUN().

Referenced by xsec_continuum_tag().

void CKD_222_self_h2o	(	MatrixView	pxsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr,
		ConstVectorView	abs_n2
	)

CKD version 2.2.2 H2O self continuum absorption model.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of H2O self continuum according to CKD_2_2_2 [1/m]
	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_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	H2O volume mixing ratio profile [1]
	abs_n2	N2 volume mixing ratio profile [1]

Note:: This absorption model is taken from the FORTRAN77 code of CKD version 2.2.2 written by
Atmospheric and Environmental Research Inc. (AER),
Radiation and Climate Group
131 Hartwell Avenue
Lexington, MA 02421, USA
http://www.rtweb.aer.com/continuum_frame.html

Author:: Thomas Kuhn

Date:: 2002-31-10

Definition at line 2098 of file continua.cc.

References addF77fields, ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, RADFN_FUN(), SL260_ckd_0, SL260_ckd_0_dv, SL260_ckd_0_npt, SL260_ckd_0_v1, SL260_ckd_0_v2, SL296_ckd_0, SL296_ckd_0_dv, SL296_ckd_0_npt, SL296_ckd_0_v1, SL296_ckd_0_v2, SPEED_OF_LIGHT, and XINT_FUN().

Referenced by xsec_continuum_tag().

void CKD_241_co2	(	MatrixView	pxsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

CKD version 2.4.1 CO2 continuum absorption model.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of CO2 continuum according to CKD_MT 1.00 [1/m]
	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_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	CO2 volume mixing ratio profile [1]

Note:: This absorption model is taken from the FORTRAN77 code of CKD version 2.4.1 written by
Atmospheric and Environmental Research Inc. (AER),
Radiation and Climate Group
131 Hartwell Avenue
Lexington, MA 02421, USA
http://www.rtweb.aer.com/continuum_frame.html

Author:: Thomas Kuhn

Date:: 2002-28-08

Definition at line 3610 of file continua.cc.

References addF77fields, FCO2_ckd_mt_100, FCO2_ckd_mt_100_dv, FCO2_ckd_mt_100_npt, FCO2_ckd_mt_100_v1, FCO2_ckd_mt_100_v2, ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, RADFN_FUN(), SPEED_OF_LIGHT, and XINT_FUN().

Referenced by xsec_continuum_tag().

void CKD_242_foreign_h2o	(	MatrixView	pxsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr,
		ConstVectorView	abs_n2
	)

CKD version 2.4.2 H2O foreign continuum absorption model.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of H2O foreign continuum according to CKDv.2.4.2 [1/m]
	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_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	H2O volume mixing ratio profile [1]
	abs_n2	N2 volume mixing ratio profile [1]

Note:: This absorption model is taken from the FORTRAN77 code of CKD version 2.4.2 written by
Atmospheric and Environmental Research Inc. (AER),
Radiation and Climate Group
131 Hartwell Avenue
Lexington, MA 02421, USA
http://www.rtweb.aer.com/continuum_frame.html

Author:: Thomas Kuhn

Date:: 2002-28-08

Definition at line 2909 of file continua.cc.

References addF77fields, FH2O_ckd_0, FH2O_ckd_0_dv, FH2O_ckd_0_npt, FH2O_ckd_0_v1, FH2O_ckd_0_v2, ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, RADFN_FUN(), SPEED_OF_LIGHT, and XINT_FUN().

Referenced by xsec_continuum_tag().

void CKD_242_self_h2o	(	MatrixView	pxsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr,
		ConstVectorView	abs_n2
	)

CKD version 2.4.2 H2O self continuum absorption model.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of H2O self continuum according to CKD_2_4_2 [1/m]
	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_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	H2O volume mixing ratio profile [1]
	abs_n2	N2 volume mixing ratio profile [1]

Note:: This absorption model is taken from the FORTRAN77 code of CKD version 2.4.2 written by
Atmospheric and Environmental Research Inc. (AER),
Radiation and Climate Group
131 Hartwell Avenue
Lexington, MA 02421, USA
http://www.rtweb.aer.com/continuum_frame.html

Author:: Thomas Kuhn

Date:: 2002-30-10

Definition at line 2609 of file continua.cc.

References addF77fields, ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, RADFN_FUN(), SL260_ckd_0, SL260_ckd_0_dv, SL260_ckd_0_npt, SL260_ckd_0_v1, SL260_ckd_0_v2, SL296_ckd_0, SL296_ckd_0_dv, SL296_ckd_0_npt, SL296_ckd_0_v1, SL296_ckd_0_v2, SPEED_OF_LIGHT, and XINT_FUN().

Referenced by xsec_continuum_tag().

void CKD_mt_100_foreign_h2o	(	MatrixView	pxsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr,
		ConstVectorView	abs_n2
	)

CKD version MT 1.00 H2O foreign continuum absorption model.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of H2O foreign continuum according to CKD_MT 1.00 [1/m]
	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_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	H2O volume mixing ratio profile [1]
	abs_n2	N2 volume mixing ratio profile [1]

Note:: This absorption model is taken from the FORTRAN77 code of CKD_MT version 1.00 written by
Atmospheric and Environmental Research Inc. (AER),
Radiation and Climate Group
131 Hartwell Avenue
Lexington, MA 02421, USA
http://www.rtweb.aer.com/continuum_frame.html

Author:: Thomas Kuhn

Date:: 2002-28-08

Definition at line 3410 of file continua.cc.

References addF77fields, FH2O_ckd_mt_100, FH2O_ckd_mt_100_dv, FH2O_ckd_mt_100_npt, FH2O_ckd_mt_100_v1, FH2O_ckd_mt_100_v2, ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, RADFN_FUN(), SPEED_OF_LIGHT, and XINT_FUN().

Referenced by xsec_continuum_tag().

void CKD_mt_100_self_h2o	(	MatrixView	pxsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr,
		ConstVectorView	abs_n2
	)

CKD version MT 1.00 H2O self continuum absorption model.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of H2O self continuum according to CKD_MT 1.00 [1/m]
	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_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	H2O volume mixing ratio profile [1]
	abs_n2	N2 volume mixing ratio profile [1]

Note:: This absorption model is taken from the FORTRAN77 code of CKD_MT version 1.00 written by
Atmospheric and Environmental Research Inc. (AER),
Radiation and Climate Group
131 Hartwell Avenue
Lexington, MA 02421, USA
http://www.rtweb.aer.com/continuum_frame.html

Author:: Thomas Kuhn

Date:: 2002-28-08

Definition at line 3153 of file continua.cc.

References addF77fields, ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, RADFN_FUN(), SL260_ckd_mt_100, SL260_ckd_mt_100_dv, SL260_ckd_mt_100_npt, SL260_ckd_mt_100_v1, SL260_ckd_mt_100_v2, SL296_ckd_mt_100, SL296_ckd_mt_100_dv, SL296_ckd_mt_100_npt, SL296_ckd_mt_100_v1, SL296_ckd_mt_100_v2, SPEED_OF_LIGHT, and XINT_FUN().

Referenced by xsec_continuum_tag().

void CKD_mt_CIAfun_n2	(	MatrixView	pxsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

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).

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of N2-N2 CIA fundamental band according to CKD_MT 1.00 [1/m]
	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_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	N2 volume mixing ratio profile [1]

Remarks:: 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)

Note:: This absorption model is taken from the FORTRAN77 code of CKD_MT version 1.00 written by
Atmospheric and Environmental Research Inc. (AER),
Radiation and Climate Group
131 Hartwell Avenue
Lexington, MA 02421, USA
http://www.rtweb.aer.com/continuum_frame.html

Author:: Thomas Kuhn

Date:: 2002-28-08

Definition at line 4269 of file continua.cc.

References addF77fields, N2N2_N2F_ckd_mt_100, N2N2_N2F_ckd_mt_100_dv, N2N2_N2F_ckd_mt_100_npt, N2N2_N2F_ckd_mt_100_v1, N2N2_N2F_ckd_mt_100_v2, N2N2_N2Ft_ckd_mt_100, ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, RADFN_FUN(), SPEED_OF_LIGHT, VMRCalcLimit, and XINT_FUN().

Referenced by xsec_continuum_tag().

void CKD_mt_CIAfun_o2	(	MatrixView	pxsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

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).

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of O2-O2 CIA fundamental band according to CKD_MT 1.00 [1/m]
	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_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	O2 volume mixing ratio profile [1]

Remarks:: 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).

Note:: This absorption model is taken from the FORTRAN77 code of CKD_MT version 1.00 written by
Atmospheric and Environmental Research Inc. (AER),
Radiation and Climate Group
131 Hartwell Avenue
Lexington, MA 02421, USA
http://www.rtweb.aer.com/continuum_frame.html

Author:: Thomas Kuhn

Date:: 2002-28-08

Definition at line 4482 of file continua.cc.

References addF77fields, ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), O2O2_O2F_ckd_mt_100_dv, O2O2_O2F_ckd_mt_100_npt, O2O2_O2F_ckd_mt_100_v1, O2O2_O2F_ckd_mt_100_v2, O2O2_O2Fo_ckd_mt_100, O2O2_O2Ft_ckd_mt_100, out3, RADFN_FUN(), SPEED_OF_LIGHT, and XINT_FUN().

Referenced by xsec_continuum_tag().

void CKD_mt_CIArot_n2	(	MatrixView	pxsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

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.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of N2-N2 CIA rot. band according to CKD_MT 1.00 [1/m]
	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_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	N2 volume mixing ratio profile [1]

Remarks:: 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.

Note:: This absorption model is taken from the FORTRAN77 code of CKD_MT version 1.00 written by
Atmospheric and Environmental Research Inc. (AER),
Radiation and Climate Group
131 Hartwell Avenue
Lexington, MA 02421, USA
http://www.rtweb.aer.com/continuum_frame.html

Author:: Thomas Kuhn

Date:: 2002-28-08

Definition at line 4018 of file continua.cc.

References addF77fields, N2N2_CT220_ckd_mt_100, N2N2_CT220_ckd_mt_100_dv, N2N2_CT220_ckd_mt_100_npt, N2N2_CT220_ckd_mt_100_v1, N2N2_CT220_ckd_mt_100_v2, N2N2_CT296_ckd_mt_100, N2N2_CT296_ckd_mt_100_dv, N2N2_CT296_ckd_mt_100_npt, N2N2_CT296_ckd_mt_100_v1, N2N2_CT296_ckd_mt_100_v2, ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, RADFN_FUN(), SPEED_OF_LIGHT, and XINT_FUN().

Referenced by xsec_continuum_tag().

void CKD_mt_co2	(	MatrixView	pxsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

CKD version MT 1.00 CO2 continuum absorption model.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of CO2 continuum according to CKD_MT 1.00 [1/m]
	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_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	CO2 volume mixing ratio profile [1]

Note:: This absorption model is taken from the FORTRAN77 code of CKD_MT version 1.00 written by
Atmospheric and Environmental Research Inc. (AER),
Radiation and Climate Group
131 Hartwell Avenue
Lexington, MA 02421, USA
http://www.rtweb.aer.com/continuum_frame.html

Author:: Thomas Kuhn

Date:: 2002-28-08

Definition at line 3806 of file continua.cc.

References addF77fields, FCO2_ckd_mt_100, FCO2_ckd_mt_100_dv, FCO2_ckd_mt_100_npt, FCO2_ckd_mt_100_v1, FCO2_ckd_mt_100_v2, ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, RADFN_FUN(), SPEED_OF_LIGHT, and XINT_FUN().

Referenced by xsec_continuum_tag().

void CKD_mt_v0v0_o2	(	MatrixView	pxsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr,
		ConstVectorView	abs_n2
	)

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).

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of O2 v0<-v0 band according to CKD_MT 1.00 [1/m]
	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_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	O2 volume mixing ratio profile [1]
	abs_n2	N2 volume mixing ratio profile [1]

Remarks:: 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.

Note:: This absorption model is taken from the FORTRAN77 code of CKD_MT version 1.00 written by
Atmospheric and Environmental Research Inc. (AER),
Radiation and Climate Group
131 Hartwell Avenue
Lexington, MA 02421, USA
http://www.rtweb.aer.com/continuum_frame.html

Oxygen band absorption model for the $a^1\Delta_g$ ← $X^3\Sigma^-_g$ band system considering the $\nu=0$ ← $\nu=0$ transitions.

Author:: Thomas Kuhn

Date:: 2002-28-08

Definition at line 4703 of file continua.cc.

References addF77fields, ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), O2_00_ckd_mt_100, O2_00_ckd_mt_100_dv, O2_00_ckd_mt_100_npt, O2_00_ckd_mt_100_v1, O2_00_ckd_mt_100_v2, out3, RADFN_FUN(), SPEED_OF_LIGHT, and XINT_FUN().

Referenced by xsec_continuum_tag().

void CKD_mt_v1v0_o2	(	MatrixView	pxsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

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.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of O2 v1<-v0 band according to CKD_MT 1.00 [1/m]
	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_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	O2 volume mixing ratio profile [1]

Remarks:: Mlawer, Clough, Brown, Stephen, Landry, Goldman, Murcray,
Observed Atmospheric Collision Induced Absorption in Near Infrared Oxygen Bands,
J. Geophys. Res., 103, D4, 3859-3863, 1998.

Note:: This absorption model is taken from the FORTRAN77 code of CKD_MT version 1.00 written by
Atmospheric and Environmental Research Inc. (AER),
Radiation and Climate Group
131 Hartwell Avenue
Lexington, MA 02421, USA
http://www.rtweb.aer.com/continuum_frame.html

Oxygen band absorption model for the $a^1\Delta_g$ ← $X^3\Sigma^-_g$ band system considering the $\nu=0$ ← $\nu=1$ transitions.

Author:: Thomas Kuhn

Date:: 2002-28-08

Definition at line 4908 of file continua.cc.

References addF77fields, ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), O2_10_ckd_mt_100_dv, O2_10_ckd_mt_100_v1, O2_10_ckd_mt_100_v2, out3, RADFN_FUN(), SPEED_OF_LIGHT, and XINT_FUN().

Referenced by xsec_continuum_tag().

void CP98H2OAbsModel	(	MatrixView	pxsec,
		const Numeric	CCin,
		const Numeric	CLin,
		const Numeric	CWin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

CP98H2OAbsModel.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of H2O (lines+continuum) according to Cruz-Pol 1998 [1/m]
	CCin	scaling factor for the H2O-continuum [1]
	CLin	scaling factor for the line strengths [1]
	CWin	scaling factor for the line widths [1]
	model	allows user defined input parameter set (CCin, CLin, and CWin) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	H2O volume mixing ratio [1]

Note:: Except for model 'user' the input parameters CCin, CLin, and CWin are neglected (model dominates over parameters).
Allowed models: 'CruzPol', 'CruzPolLines', 'CruzPolContinuum', and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: S. L. Cruz-Pol et al., Radio Science, 33(5), 1319, 1998.

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 1512 of file continua.cc.

References Hz_to_GHz, MPMLineShapeFunction(), ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, Pa_to_hPa, and VMRCalcLimit.

Referenced by xsec_continuum_tag().

void MaTipping_H2O_foreign_continuum	(	MatrixView	pxsec,
		const Numeric	Cin,
		const Numeric	xin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

MaTipping_H2O_foreign_continuum.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of the H2O-dry air continuum [1/m]
	Cin	constant absorption strength [1/m / (Hz*Pa)�]
	xin	temperature exponent [1]
	model	allows user defined input parameter set (C and x) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure [Pa]
	abs_t	predefined temperature grid [K]
	vmr	H2O volume mixing ratio [1]

Note:: Except for model 'user' the input parameters C and x are neglected (model dominates over parameters).
Allowed models: 'MaTipping', and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: Q. Ma and R. H. Tipping, J. Chem. Phys., 117(23), 10581, 2002.

Author:: Thomas Kuhn

Date:: 2002-12-04

Definition at line 1886 of file continua.cc.

References ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), and out3.

Referenced by xsec_continuum_tag().

void MPM85O2AbsModel	(	MatrixView	pxsec,
		const Numeric	CCin,
		const Numeric	CLin,
		const Numeric	CWin,
		const Numeric	COin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	abs_h2o,
		ConstVectorView	vmr
	)

MPM85O2AbsModel.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of O2 according to MPM89 [1/m]
	CCin	scaling factor for the O2-continuum [1]
	CLin	scaling factor for the O2-line strengths [1]
	CWin	scaling factor for the O2-line widths [1]
	COin	scaling factor for the O2-line coupling [1]
	model	allows user defined input parameter set (CCin, CLin, CWin, and COin) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure [Pa]
	abs_t	predefined temperature grid [K]
	abs_h2o	H2O volume mixing ratio profile [1]
	vmr	O2 volume mixing ratio profile [1]

Note:: Except for model 'user' the input parameters CCin, CLin, CWin, and COin are neglected (model dominates over parameters).
Allowed models: 'MPM85', 'MPM85Lines', 'MPM85Continuum', 'MPM85NoCoupling', 'MPM85NoCutoff', and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: H. J. Liebe,
An updated model for millimeter wave propagation in moist air,,
Radio Science, vol. 20, pp. 1069-1089, 1985

Author:: Thomas Kuhn

Date:: 2002-04-05

Definition at line 5559 of file continua.cc.

References dB_km_to_1_m, Hz_to_GHz, MPMLineShapeO2Function(), ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, Pa_to_kPa, and VMRCalcLimit.

Referenced by xsec_continuum_tag().

void MPM87H2OAbsModel	(	MatrixView	pxsec,
		const Numeric	CCin,
		const Numeric	CLin,
		const Numeric	CWin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

MPM87H2OAbsModel.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of H2O (lines+continuum) according to MPM87 [1/m]
	CCin	scaling factor for the H2O-continuum [1]
	CLin	scaling factor for the H2O-line strengths [1]
	CWin	scaling factor for the H2O-line widths [1]
	model	allows user defined input parameter set (CCin, CLin, and CWin) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	H2O volume mixing ratio [1]

Note:: Except for model 'user' the input parameters CCin, CLin, and CWin are neglected (model dominates over parameters).
Allowed models: 'MPM87', 'MPM87Lines', 'MPM87Continuum', and 'user'. See the user guide for detailed explanations.

Remarks:: H. J. Liebe,
A contribution to modeling atmospheric millimeter-wave properties,
Frequenz, 41, 1987, 31-36
and
H. J. Liebe and D. H. Layton,
Millimeter-wave properties of the atmosphere: Laboratory studies and propagation modeling,
U.S. Dept. of Commerce, National Telecommunications and Information Administration, Institute for Communication Sciences,
325 Broadway, Boulder, CO 80303-3328, report 87224.

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 441 of file continua.cc.

References dB_km_to_1_m, Hz_to_GHz, MPMLineShapeFunction(), ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, and Pa_to_kPa.

Referenced by xsec_continuum_tag().

void MPM87O2AbsModel	(	MatrixView	pxsec,
		const Numeric	CCin,
		const Numeric	CLin,
		const Numeric	CWin,
		const Numeric	COin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	abs_h2o,
		ConstVectorView	vmr
	)

MPM87O2AbsModel.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of O2 according to MPM89 [1/m]
	CCin	scaling factor for the O2-continuum [1]
	CLin	scaling factor for the O2-line strengths [1]
	CWin	scaling factor for the O2-line widths [1]
	COin	scaling factor for the O2-line coupling [1]
	model	allows user defined input parameter set (CCin, CLin, CWin, and COin) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure [Pa]
	abs_t	predefined temperature grid [K]
	abs_h2o	H2O volume mixing ratio profile [1]
	vmr	O2 volume mixing ratio profile [1]

Note:: Except for model 'user' the input parameters CCin, CLin, CWin, and COin are neglected (model dominates over parameters).
Allowed models: 'MPM87', 'MPM87Lines', 'MPM87Continuum', 'MPM87NoCoupling', 'MPM87NoCutoff', and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: H. J. Liebe and D. H. Layton,
Millimeter-wave properties of the atmosphere: Laboratory studies and propagation modelling,
U.S. Dept. of Commerce, National Telecommunications and Information Administration, Institute for Communication Sciences, rep. 87-224,
325 Broadway, Boulder, CO 80303-3328

Author:: Thomas Kuhn

Date:: 2002-04-05

Definition at line 5841 of file continua.cc.

References dB_km_to_1_m, Hz_to_GHz, MPMLineShapeO2Function(), ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, Pa_to_kPa, and VMRCalcLimit.

Referenced by xsec_continuum_tag().

void MPM89H2OAbsModel	(	MatrixView	pxsec,
		const Numeric	CCin,
		const Numeric	CLin,
		const Numeric	CWin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

MPM89H2OAbsModel.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of H2O (lines+continuum) according to MPM89 [1/m]
	CCin	scaling factor for the H2O-continuum [1]
	CLin	scaling factor for the line strengths [1]
	CWin	scaling factor for the line widths [1]
	model	allows user defined input parameter set (CCin, CLin, and CWin) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	H2O volume mixing ratio [1]

Note:: Except for model 'user' the input parameters CCin, CLin, and CWin are neglected (model dominates over parameters).
Allowed models: 'MPM89', 'MPM89Lines', 'MPM89Continuum', and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: H. J. Liebe, Int. J. Infrared and Millimeter Waves, 10(6), 1989, 631.

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 624 of file continua.cc.

References dB_km_to_1_m, Hz_to_GHz, MPMLineShapeFunction(), ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, and Pa_to_kPa.

Referenced by xsec_continuum_tag().

void MPM89O2AbsModel	(	MatrixView	pxsec,
		const Numeric	CCin,
		const Numeric	CLin,
		const Numeric	CWin,
		const Numeric	COin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	abs_h2o,
		ConstVectorView	vmr
	)

MPM89O2AbsModel.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of O2 according to MPM89 [1/m]
	CCin	scaling factor for the O2-continuum [1]
	CLin	scaling factor for the O2-line strengths [1]
	CWin	scaling factor for the O2-line widths [1]
	COin	scaling factor for the O2-line coupling [1]
	model	allows user defined input parameter set (CCin, CLin, CWin, and COin) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure [Pa]
	abs_t	predefined temperature grid [K]
	abs_h2o	H2O volume mixing ratio profile [1]
	vmr	O2 volume mixing ratio profile [1]

Note:: Except for model 'user' the input parameters CCin, CLin, CWin, and COin are neglected (model dominates over parameters).
Allowed models: 'MPM89', 'MPM89Lines', 'MPM89Continuum', 'MPM89NoCoupling', 'MPM89NoCutoff', and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: H. J. Liebe,
MPM - an atmospheric millimeter-wave propagation model,
Int. J. Infrared and Mill. Waves, Vol 10, pp. 631-650, 1989.

Author:: Thomas Kuhn

Date:: 2002-04-05

Definition at line 6115 of file continua.cc.

References dB_km_to_1_m, Hz_to_GHz, MPMLineShapeO2Function(), ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, Pa_to_kPa, and VMRCalcLimit.

Referenced by xsec_continuum_tag().

void MPM92O2AbsModel	(	MatrixView	pxsec,
		const Numeric	CCin,
		const Numeric	CLin,
		const Numeric	CWin,
		const Numeric	COin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	abs_h2o,
		ConstVectorView	vmr
	)

MPM92O2AbsModel.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of O2 according to MPM93 [1/m]
	CCin	scaling factor for the O2-continuum [1]
	CLin	scaling factor for the O2-line strengths [1]
	CWin	scaling factor for the O2-line widths [1]
	COin	scaling factor for the O2-line coupling [1]
	model	allows user defined input parameter set (CCin, CLin, CWin, and COin) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure [Pa]
	abs_t	predefined temperature grid [K]
	abs_h2o	H2O volume mixing ratio profile [1]
	vmr	O2 volume mixing ratio profile [1]

Note:: Except for model 'user' the input parameters CCin, CLin, CWin, and COin are neglected (model dominates over parameters).
Allowed models: 'MPM92', 'MPM92Lines', 'MPM92Continuum', 'MPM92NoCoupling', 'MPM92NoCutoff', and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: 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

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 6384 of file continua.cc.

References dB_km_to_1_m, Hz_to_GHz, MPMLineShapeO2Function(), ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, Pa_to_hPa, and VMRCalcLimit.

Referenced by xsec_continuum_tag().

void MPM93_H2O_continuum	(	MatrixView	pxsec,
		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_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

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/

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of H2O according to MPM87 [1/m]
	fcenter	continuum pseudo-line center frequency [Hz]
	b1	continuum pseudo-line line strength [Hz/Pa]
	b2	continuum pseudo-line line strength temperature exponent [1]
	b3	continuum pseudo-line line broadening parameter [Hz/Pa]
	b4	continuum pseudo-line line broadening parameter [1]
	b5	continuum pseudo-line line broadening parameter [1]
	b6	continuum pseudo-line line broadening parameter [1]
	model	allows user defined input parameter set (fcenter and b1 to b6) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	H2O volume mixing ratio [1]

Note:: Except for model 'user' the input parameters fcenter and b1 to b6 are neglected (model dominates over parameters).
Allowed models: 'MPM93' and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: 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

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 5422 of file continua.cc.

References dB_km_to_1_m, MPMLineShapeFunction(), ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), and out3.

Referenced by xsec_continuum_tag().

void MPM93_N2_continuum	(	MatrixView	pxsec,
		const Numeric	Cin,
		const Numeric	Gin,
		const Numeric	xTin,
		const Numeric	xfin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	abs_h2o,
		ConstVectorView	vmr
	)

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/

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of N2-continuum according to MPM93 [1/m]
	Cin	continuum strength [ppm/GHz]
	Gin	width parameter [Hz/Pa]
	xTin	continuum strength temperature exponent [1]
	xfin	continuum frequency exponent [1]
	model	allows user defined input parameter set (Cin, Gin, xTin, and xfin) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	abs_h2o	H2O volume mixing ratio profile [1]
	vmr	N2 volume mixing ratio profile [1]

Note:: Except for model 'user' the input parameters Cin, Gin, xTin, and xfin are neglected (model dominates over parameters).
Allowed models: 'MPM93' and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: 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

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 7875 of file continua.cc.

References fac(), ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, PI, and SPEED_OF_LIGHT.

Referenced by xsec_continuum_tag().

void MPM93_O2_continuum	(	MatrixView	pxsec,
		const Numeric	S0in,
		const Numeric	G0in,
		const Numeric	XS0in,
		const Numeric	XG0in,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	abs_h2o,
		ConstVectorView	vmr
	)

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/

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of O2-continuum according to MPM93 [1/m]
	S0in	O2-continuum strength [1/Pa]
	G0in	O2-continuum width [Hz/Pa]
	XS0in	O2-continuum strength temperature exponent [1]
	XG0in	O2-continuum width temperature exponent [1]
	model	allows user defined input parameter set (S0in, G0in, xS0in, and xG0in) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	abs_h2o	H2O volume mixing ratio profile [1]
	vmr	O2 volume mixing ratio profile [1]

Note:: Except for model 'user' the input parameters S0in, G0in, xS0in, and xG0in are neglected (model dominates over parameters).
Allowed models: 'MPM93' and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: 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

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 7313 of file continua.cc.

References ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, PI, SPEED_OF_LIGHT, and VMRCalcLimit.

Referenced by xsec_continuum_tag().

void MPM93H2OAbsModel	(	MatrixView	pxsec,
		const Numeric	CCin,
		const Numeric	CLin,
		const Numeric	CWin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

MPM93H2OAbsModel.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of H2O (lines+continuum) according to MPM93 [1/m]
	CCin	scaling factor for the H2O-continuum [1]
	CLin	scaling factor for the line strengths [1]
	CWin	scaling factor for the line widths [1]
	model	allows user defined input parameter set (CCin, CLin, and CWin) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	H2O volume mixing ratio [1]

Note:: Except for model 'user' the input parameters CCin, CLin, and CWin are neglected (model dominates over parameters).
Allowed models: 'MPM93', 'MPM93Lines', 'MPM93Continuum', and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: 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

Attention:: The H2O lines at 547.676440 GHz and 552.020960 GHz are isotopic lines:
547 GHz is from the isotope 1-8-1 (HITRAN code 181, JPL code 20003) with an isotopic ratio of 0.00199983 and
552 GHz is from the isotope 1-7-1 (HITRAN code 171, JPL code 19003) with an isotopic ratio of 0.00037200.
The original source code of MPM93 has these isotopic ratios not included in the line strength parameter b1, which is an error.
In the arts implementation the line strength parameter b1 of these two lines is multiplied with the appropriate isotopic ratio.

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 1082 of file continua.cc.

References dB_km_to_1_m, Hz_to_GHz, MPMLineShapeFunction(), ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, and Pa_to_hPa.

Referenced by xsec_continuum_tag().

void MPM93IceCrystalAbs	(	MatrixView	pxsec,
		const Numeric	CCin,
		const Numeric	CAin,
		const Numeric	CBin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

MPM93IceCrystalAbs.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of ice clouds according to MPM93 [1/m]
	CCin	scaling parameter of the calculated cross section [1]
	CAin	scaling parameter of the permittivity function a (see page 3-6 in the reference) [1]
	CBin	scaling parameter of the permittivity function b (see page 3-6 in the reference) [1]
	model	allows user defined input parameter (CCin, CAin, CBin) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	suspended water droplet density profile (valid range: 0-0.001) [kg/m�]

Note:: Except for model 'user' the input parameters CCin, CAin, and CBin are neglected (model dominates over parameters).
Allowed models: 'MPM93' and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: 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.

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 8701 of file continua.cc.

References dB_km_to_1_m, Hz_to_GHz, ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), and out3.

Referenced by xsec_continuum_tag().

void MPM93O2AbsModel	(	MatrixView	pxsec,
		const Numeric	CCin,
		const Numeric	CLin,
		const Numeric	CWin,
		const Numeric	COin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	abs_h2o,
		ConstVectorView	vmr
	)

MPM93O2AbsModel.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of O2 according to MPM93 [1/m]
	CCin	scaling factor for the O2-continuum [1]
	CLin	scaling factor for the O2-line strengths [1]
	CWin	scaling factor for the O2-line widths [1]
	COin	scaling factor for the O2-line coupling [1]
	model	allows user defined input parameter set (CCin, CLin, CWin, and COin) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure [Pa]
	abs_t	predefined temperature grid [K]
	abs_h2o	H2O volume mixing ratio profile [1]
	vmr	O2 volume mixing ratio profile [1]

Note:: Except for model 'user' the input parameters CCin, CLin, CWin, and COin are neglected (model dominates over parameters).
Allowed models: 'MPM93', 'MPM93Lines', 'MPM93Continuum', 'MPM93NoCoupling', 'MPM93NoCutoff', and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: 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

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 6652 of file continua.cc.

References dB_km_to_1_m, Hz_to_GHz, MPMLineShapeO2Function(), ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, Pa_to_hPa, and VMRCalcLimit.

Referenced by xsec_continuum_tag().

void MPM93RainExt	(	MatrixView	pxsec,
		const Numeric	CEin,
		const Numeric	CAin,
		const Numeric	CBin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

MPM93RainExt.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of water clouds according to MPM93 [1/m]
	CEin	scaling parameter of the calculated cross section [1]
	CAin	scaling parameter of the factor a_rain [1]
	CBin	scaling parameter of the exponent b_rain [1]
	model	allows user defined input parameter (CEin, CAin, CBin) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	rain rate vector (i.e. vertical profile), (valid range: 0-150) [mm/h]

Note:: Except for model 'user' the input parameters CEin, CAin, and CBin are neglected (model dominates over parameters).
Allowed models: 'MPM93' and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: R. L. Olsen and 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.

Author:: Christian Melsheimer

Date:: 2003-22-05

Definition at line 8862 of file continua.cc.

References dB_km_to_1_m, Hz_to_GHz, ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), and out3.

Referenced by xsec_continuum_tag().

void MPM93WaterDropletAbs	(	MatrixView	pxsec,
		const Numeric	CCin,
		const Numeric	CGin,
		const Numeric	CEin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

MPM93WaterDropletAbs.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of water clouds according to MPM93 [1/m]
	CCin	scaling parameter of the calculated cross section [1]
	CGin	scaling parameter of the first relaxation frequency (gamma_1, see page 3-6 in the reference) [1]
	CEin	scaling parameter of the first permittivity component (epsilon_0, see page 3-6 in the reference) [1]
	model	allows user defined input parameter (CCin, CGin, CEin) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	suspended water droplet density profile (valid range: 0-0.001) [kg/m�]

Note:: Except for model 'user' the input parameters CCin, CGin, and CEin are neglected (model dominates over parameters).
Allowed models: 'MPM93' and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: 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.

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 8526 of file continua.cc.

References dB_km_to_1_m, Hz_to_GHz, ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), and out3.

Referenced by xsec_continuum_tag().

Numeric MPMLineShapeFunction	(	const Numeric	gamma,
		const Numeric	fl,
		const Numeric	f
	)

Return values:

MPMLineShapeFunction

H2O-line shape function value [1/Hz]

Parameters:

	gamma	H2O-line width [Hz]
	fl	H2O-line central frequency [Hz]
	f	frequency position of calculation [Hz]

Note:: This function calculates the line shape function of Van Vleck and Weisskopf with the factor (f/fl)�. for the MPM pseudo continuum line.

Remarks:: Reference: 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

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 9137 of file continua.cc.

Referenced by CP98H2OAbsModel(), MPM02H2OAbsModel(), MPM87H2OAbsModel(), MPM89H2OAbsModel(), MPM93_H2O_continuum(), and MPM93H2OAbsModel().

Numeric MPMLineShapeO2Function	(	const Numeric	gamma,
		const Numeric	fl,
		const Numeric	f,
		const Numeric	delta
	)

Return values:

MPMLineShapeO2Function

O2-line shape function value [1]

Parameters:

	gamma	O2-line width [Hz]
	fl	H2O-line central frequency of the [Hz]
	f	frequency position of calculation [Hz]
	delta	O2-line mixing parameter [1]

Note:: This function calculates the line shape function of Van Vleck and Weisskopf for O2 with line mixing.

Remarks:: Reference: 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

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 9194 of file continua.cc.

Referenced by MPM85O2AbsModel(), MPM87O2AbsModel(), MPM89O2AbsModel(), MPM92O2AbsModel(), and MPM93O2AbsModel().

void Pardo_ATM_H2O_ForeignContinuum	(	MatrixView	pxsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

Pardo_ATM_H2O_ForeignContinuum.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of N2-continuum according to Rosenkranz, 1993 [1/m]
	Cin	continuum strength [1/m * 1/(Hz*Pa)�]
	model	allows user defined input parameter set (Cin and xTin) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	H2O volume mixing ratio [1]

Note:: Except for model 'user' the input parameters Cin and xTin are neglected (model dominates over parameters).
Allowed models: 'ATM', and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: Pardo et al., IEEE, Trans. Ant. Prop.,
Vol 49, No 12, pp. 1683-1694, 2001.

Author:: Thomas Kuhn

Date:: 2001-04-10

Definition at line 5309 of file continua.cc.

References ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), and out3.

Referenced by xsec_continuum_tag().

void Pardo_ATM_N2_dry_continuum	(	MatrixView	pxsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr,
		ConstVectorView	h2ovmr
	)

Pardo_ATM_N2_dry_continuum.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of N2-continuum according to Rosenkranz, 1993 [1/m]
	Cin	continuum strength [1/m * 1/(Hz*Pa)�]
	model	allows user defined input parameter set (Cin and xTin) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	N2 volume mixing ratio [1]
	h2ovmr	H2O volume mixing ratio [1]

Note:: Except for model 'user' the input parameters Cin and xTin are neglected (model dominates over parameters).
Allowed models: 'ATM', and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: Pardo et al., IEEE, Trans. Ant. Prop.,
Vol 49, No 12, pp. 1683-1694, 2001.

Author:: Thomas Kuhn

Date:: 2001-04-10

Definition at line 8007 of file continua.cc.

References ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, and VMRCalcLimit.

Referenced by xsec_continuum_tag().

void PWR93O2AbsModel	(	MatrixView	pxsec,
		const Numeric	CCin,
		const Numeric	CLin,
		const Numeric	CWin,
		const Numeric	COin,
		const String &	model,
		const String &	version,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmrh2o,
		ConstVectorView	vmr
	)

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

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of O2 according to the P. W. Rosenkranz, 1993 [1/m]
	CCin	O2-continuum scale factor [1]
	CLin	O2 line strength scale factor [1]
	CWin	O2 line broadening scale factor [1]
	COin	O2 line coupling scale factor [1]
	model	allows user defined input parameter set (CCin, CLin, CWin, and COin) or choice of pre-defined parameters of specific models (see note below).
	version	determines model version: 1988, 1993, 1998
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure [Pa]
	abs_t	predefined temperature grid [K]
	vmrh2o	H2O volume mixing ratio profile [1]
	vmr	O2 volume mixing ratio profile [1]

Note:: Except for model 'user' the input parameters CCin, CLin, CWin, and COin are neglected (model dominates over parameters).
Allowed models:
'Rosenkranz', 'RosenkranzLines', 'RosenkranzContinuum', 'RosenkranzNoCoupling', and 'user'.
For the parameter version the following three string values are allowed: 'PWR88', 'PWR93', 'PWR98'.
See the user guide for detailed explanations.

Remarks:: Reference: P. W. Rosenkranz, Chapter 2, in M. A. Janssen,
Atmospheric Remote Sensing by Microwave Radiometry,
John Wiley & Sons, Inc., 1993.

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 6947 of file continua.cc.

References Hz_to_GHz, ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, Pa_to_hPa, PI, and VMRCalcLimit.

Referenced by xsec_continuum_tag().

void PWR98H2OAbsModel	(	MatrixView	pxsec,
		const Numeric	CCin,
		const Numeric	CLin,
		const Numeric	CWin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

PWR98H2OAbsModel.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of H2O (lines+continuum) according to P. W. Rosenkranz, 1998 [1/m]
	CCin	scaling factor for the H2O-continuum [1]
	CLin	scaling factor for the line strengths [1]
	CWin	scaling factor for the line widths [1]
	model	allows user defined input parameter set (CCin, CLin, and CWin) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	H2O volume mixing ratio [1]

Note:: Except for model 'user' the input parameters CCin, CLin, and CWin are neglected (model dominates over parameters).
Allowed models: 'Rosenkranz', 'RosenkranzLines', 'RosenkranzContinuum', and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: P. W. Rosenkranz., Radio Science, 33(4), 919, 1998 and Radio Science, Vol. 34(4), 1025, 1999.

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 1305 of file continua.cc.

References Hz_to_GHz, ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, and Pa_to_hPa.

Referenced by xsec_continuum_tag().

void Rosenkranz_CO2_foreign_continuum	(	MatrixView	pxsec,
		const Numeric	Cin,
		const Numeric	xin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	abs_n2,
		ConstVectorView	vmr
	)

Rosenkranz_CO2_foreign_continuum.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of CO2-N2-continuum according to Rosenkranz, 1993 [1/m]
	Cin	continuum strength [1/m * 1/(Hz*Pa)�]
	xin	continuum temperature exponent [1]
	model	allows user defined input parameter set (Cin and xin) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	abs_n2	N2 volume mixing ratio profile [1]
	vmr	CO2 volume mixing ratio profile [1]

Note:: Except for model 'user' the input parameters Cin and xin are neglected (model dominates over parameters).
Allowed models: 'Rosenkranz' and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: P. W. Rosenkranz, Chapter 2, pp 74, in M. A. Janssen,
Atmospheric Remote Sensing by Microwave Radiometry,
John Wiley & Sons, Inc., 1993.

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 8422 of file continua.cc.

References ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), and out3.

Referenced by xsec_continuum_tag().

void Rosenkranz_CO2_self_continuum	(	MatrixView	pxsec,
		const Numeric	Cin,
		const Numeric	xin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

Rosenkranz_CO2_self_continuum.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of CO2-CO2-continuum according to Rosenkranz, 1993 [1/m]
	Cin	continuum strength [1/m * 1/(Hz*Pa)�]
	xin	continuum temperature exponent [1]
	model	allows user defined input parameter set (Cin and xin) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	CO2 volume mixing ratio [1]

Note:: Except for model 'user' the input parameters Cin and xin are neglected (model dominates over parameters).
Allowed models: 'Rosenkranz' and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: P. W. Rosenkranz, Chapter 2, pp 74, pp 74, in M. A. Janssen,
Atmospheric Remote Sensing by Microwave Radiometry,
John Wiley & Sons, Inc., 1993.

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 8324 of file continua.cc.

References ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), and out3.

Referenced by xsec_continuum_tag().

void Rosenkranz_N2_self_continuum	(	MatrixView	pxsec,
		const Numeric	Cin,
		const Numeric	xin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

Rosenkranz_N2_self_continuum.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of N2-continuum according to Rosenkranz, 1993 [1/m]
	Cin	continuum strength [1/m * 1/(Hz*Pa)�]
	xin	temperature exponent of N2-continuum [1]
	model	allows user defined input parameter set (Cin and xTin) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	H2O volume mixing ratio [1]

Note:: Except for model 'user' the input parameters Cin and xTin are neglected (model dominates over parameters).
Allowed models: 'Rosenkranz', and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: P. W. Rosenkranz, Chapter 2, pp 74, in M. A. Janssen,
Atmospheric Remote Sensing by Microwave Radiometry,
John Wiley & Sons, Inc., 1993.

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 8109 of file continua.cc.

References ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), and out3.

Referenced by xsec_continuum_tag().

void Rosenkranz_O2_continuum	(	MatrixView	pxsec,
		const Numeric	S0in,
		const Numeric	G0in,
		const Numeric	XS0in,
		const Numeric	XG0in,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	abs_h2o,
		ConstVectorView	vmr
	)

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

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of O2-continuum according to Rosenkranz 1993 [1/m]
	S0in	line strength [K�/(HzPam)]
	G0in	line width [Hz/Pa]
	XS0in	line strength temperature exponent [1]
	XG0in	line widths temperature exponent [1]
	model	allows user defined input parameter set (S0in, G0in, XS0in, and XG0in) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	abs_h2o	H2O volume mixing ratio profile [1]
	vmr	O2 volume mixing ratio profile [1]

Note:: Except for model 'user' the input parameters S0in, G0in, XS0in, and XG0in are neglected (model dominates over parameters).
Allowed models: 'Rosenkranz' and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: P. W. Rosenkranz, Chapter 2, in M. A. Janssen,
Atmospheric Remote Sensing by Microwave Radiometry,
John Wiley & Sons, Inc., 1993.

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 7459 of file continua.cc.

References ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), and out3.

Referenced by xsec_continuum_tag().

void Standard_H2O_foreign_continuum	(	MatrixView	pxsec,
		const Numeric	Cin,
		const Numeric	xin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

Standard_H2O_foreign_continuum.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of the H2O-dry air continuum [1/m]
	Cin	constant absorption strength [1/m / (Hz*Pa)�]
	xin	temperature exponent [1]
	model	allows user defined input parameter set (C and x) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_t	predefined temperature grid [K]
	abs_p	predefined pressure [Pa]
	vmr	H2O volume mixing ratio [1]

Note:: Except for model 'user' the input parameters C and x are neglected (model dominates over parameters).
Allowed models: 'Rosenkranz', 'CruzPol', 'MPM89', 'MPM87', and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: P. W. Rosenkranz., Radio Science, 33(4), 919, 1998 and Radio Science, Vol. 34(4), 1025, 1999.

Author:: Thomas Kuhn

Date:: 2001-08-03

Definition at line 1764 of file continua.cc.

References ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), and out3.

Referenced by xsec_continuum_tag().

void Standard_H2O_self_continuum	(	MatrixView	pxsec,
		const Numeric	Cin,
		const Numeric	xin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

Standard_H2O_self_continuum.

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of the H2O-H2O continuum [1/m]
	Cin	constant absorption strength [1/m / (Hz*Pa)�]
	xin	temperature exponent of (300/T) [1]
	model	allows user defined input parameter set (C and x) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	H2O volume mixing ratio [1]

Note:: Except for model 'user' the input parameters C and x are neglected (model dominates over parameters).
Allowed models: 'Rosenkranz', 'CruzPol', 'MPM89', 'MPM87', and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: P. W. Rosenkranz., Radio Science, 33(4), 919, 1998 and Radio Science, Vol. 34(4), 1025, 1999.

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 1642 of file continua.cc.

References ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), and out3.

Referenced by xsec_continuum_tag().

void Standard_N2_self_continuum	(	MatrixView	pxsec,
		const Numeric	Cin,
		const Numeric	xfin,
		const Numeric	xtin,
		const Numeric	xpin,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	vmr
	)

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

Parameters:

`[out]`	pxsec	cross section (absorption/volume mixing ratio) of N2-continuum according to Rosenkranz, 1993 [1/m]
	Cin	continuum strength [1/m * 1/(Hz*Pa)�]
	xfin	continuum frequency exponent [1]
	xtin	continuum strength temperature exponent [1]
	xpin	continuum strength pressure exponent [1]
	model	allows user defined input parameter set (Cin, xfin, xtin, and xpin) or choice of pre-defined parameters of specific models (see note below).
	f_grid	predefined frequency grid [Hz]
	abs_p	predefined pressure grid [Pa]
	abs_t	predefined temperature grid [K]
	vmr	H2O volume mixing ratio [1]

Note:: Except for model 'user' the input parameters Cin, xfin, xtin, and xpin are neglected (model dominates over parameters).
Allowed models: 'Rosenkranz', and 'user'. See the user guide for detailed explanations.

Remarks:: Reference: P. W. Rosenkranz, Chapter 2, in M. A. Janssen,
Atmospheric Remote Sensing by Microwave Radiometry,
John Wiley & Sons, Inc., 1993.

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 8212 of file continua.cc.

References ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), and out3.

Referenced by xsec_continuum_tag().

Numeric WVSatPressureIce ( const Numeric t )

Return values:

WVSatPressureIce

water vapor saturation pressure over liquid water [Pa]

Parameters:

t

temperature [K]

Note:: This function calculates the water vapor saturation pressure over ice water according to the Goff-Gratch equation. Other links:
Global Atmospheric Water Balance
Schlatter (profsc.fsl.noaa.gov)

Remarks:: Reference: 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

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 9319 of file continua.cc.

Numeric WVSatPressureLiquidWater ( const Numeric t )

Return values:

WVSatPressureLiquidWater

water vapor saturation pressure over liquid water [Pa]

Parameters:

t

temperature [K]

Note:: This function calculates the water vapor saturation pressure over liquid water according to the Goff-Gratch equation.
Other links:
Global Atmospheric Water Balance
Schlatter (profsc.fsl.noaa.gov)

Remarks:: Reference: 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

Author:: Thomas Kuhn

Date:: 2001-11-05

Definition at line 9254 of file continua.cc.

void xsec_continuum_tag	(	MatrixView	xsec,
		const String &	name,
		ConstVectorView	parameters,
		const String &	model,
		ConstVectorView	f_grid,
		ConstVectorView	abs_p,
		ConstVectorView	abs_t,
		ConstVectorView	abs_n2,
		ConstVectorView	abs_h2o,
		ConstVectorView	vmr
	)

Calculates model absorption for one continuum or full model tag.

Note, that only one tag can be taken at a time.

Calculated is the true absorption cross section, that means you have to multiply this with n*VMR in order to get the absorption coefficient in units of 1/m.

This is the type of xsec that is used all over ARTS, but not what is used by the internal continuum functions! (We have to divide the output of the internal continuum functions by the number density n.)

Return values:

xsec

Cross section of one continuum tag,
xsec = alpha / (n*VMR) [m^2]. This is both input and output! (The function adds the continuum absorption cross section to the previous content of xsec.)

Parameters:

	name	The name of the model to calculate (derived from the tag name)
	parameters	model parameters, as defined in method abs_cont_parameters.
	model	model, related to model parameters
	f_grid	Frequency grid [Hz]
	abs_p	Pressure grid [Pa]
	abs_t	Temperatures associated with the pressure grid, abs_p [K]
	abs_n2	Total volume mixing ratio profile of molecular nitrogen. This will be needed only for the CO2 foreign continuum [1] however one is forced to give this input [1]
	abs_h2o	Total volume mixing ratio profile of water vapor. This will be needed only for the oxygen continuum however one is forced to give this input [1]
	vmr	Volume mixing ratio profile of the actual species [1]

Author:: Stefan B�hler, Thomas Kuhn

Date:: 2001-11-05

Definition at line 9385 of file continua.cc.

References BF86_CIA_N2(), BOLTZMAN_CONST, CKD24_H20(), CKD_222_foreign_h2o(), CKD_222_self_h2o(), CKD_241_co2(), CKD_242_foreign_h2o(), CKD_242_self_h2o(), CKD_mt_100_foreign_h2o(), CKD_mt_100_self_h2o(), CKD_mt_CIAfun_n2(), CKD_mt_CIAfun_o2(), CKD_mt_CIArot_n2(), CKD_mt_co2(), CKD_mt_v0v0_o2(), CKD_mt_v1v0_o2(), CP98H2OAbsModel(), joker, MaTipping_H2O_foreign_continuum(), MPM85O2AbsModel(), MPM87H2OAbsModel(), MPM87O2AbsModel(), MPM89H2OAbsModel(), MPM89O2AbsModel(), MPM92O2AbsModel(), MPM93_H2O_continuum(), MPM93_N2_continuum(), MPM93_O2_continuum(), MPM93H2OAbsModel(), MPM93IceCrystalAbs(), MPM93O2AbsModel(), MPM93RainExt(), MPM93WaterDropletAbs(), ConstMatrixView::ncols(), ConstVectorView::nelem(), ConstMatrixView::nrows(), out3, Pardo_ATM_H2O_ForeignContinuum(), Pardo_ATM_N2_dry_continuum(), PWR93O2AbsModel(), PWR98H2OAbsModel(), Rosenkranz_CO2_foreign_continuum(), Rosenkranz_CO2_self_continuum(), Rosenkranz_N2_self_continuum(), Rosenkranz_O2_continuum(), Standard_H2O_foreign_continuum(), Standard_H2O_self_continuum(), Standard_N2_self_continuum(), and Standard_O2_continuum().

Referenced by abs_xsec_per_speciesAddConts().

Variable Documentation

const int addF77fields = 1

Definition at line 534 of file continua.h.

Referenced by CKD_222_foreign_h2o(), CKD_222_self_h2o(), CKD_241_co2(), CKD_242_foreign_h2o(), CKD_242_self_h2o(), CKD_mt_100_foreign_h2o(), CKD_mt_100_self_h2o(), CKD_mt_CIAfun_n2(), CKD_mt_CIAfun_o2(), CKD_mt_CIArot_n2(), CKD_mt_co2(), CKD_mt_v0v0_o2(), and CKD_mt_v1v0_o2().

const double FCO2_ckd_mt_100[FCO2_ckd_mt_100_npt+addF77fields]

Definition at line 3072 of file continua.h.

Referenced by CKD_241_co2(), and CKD_mt_co2().

const Numeric FCO2_ckd_mt_100_dv = 10.0

Definition at line 3070 of file continua.h.

Referenced by CKD_241_co2(), and CKD_mt_co2().

const int FCO2_ckd_mt_100_npt = 1003

Definition at line 3071 of file continua.h.

Referenced by CKD_241_co2(), and CKD_mt_co2().

const Numeric FCO2_ckd_mt_100_v1 = -20.0

Definition at line 3068 of file continua.h.

Referenced by CKD_241_co2(), and CKD_mt_co2().

const Numeric FCO2_ckd_mt_100_v2 = 10000.0

Definition at line 3069 of file continua.h.

Referenced by CKD_241_co2(), and CKD_mt_co2().

const double FH2O_ckd_0[FH2O_ckd_0_npt+addF77fields]

Definition at line 975 of file continua.h.

Referenced by CKD_222_foreign_h2o(), and CKD_242_foreign_h2o().

const Numeric FH2O_ckd_0_dv = 10.0

Definition at line 973 of file continua.h.

Referenced by CKD_222_foreign_h2o(), and CKD_242_foreign_h2o().

const int FH2O_ckd_0_npt = 2003

Definition at line 974 of file continua.h.

Referenced by CKD_222_foreign_h2o(), and CKD_242_foreign_h2o().

const Numeric FH2O_ckd_0_v1 = -20.0

Definition at line 971 of file continua.h.

Referenced by CKD_222_foreign_h2o(), and CKD_242_foreign_h2o().

const Numeric FH2O_ckd_0_v2 = 20000.0

Definition at line 972 of file continua.h.

Referenced by CKD_222_foreign_h2o(), and CKD_242_foreign_h2o().

const double FH2O_ckd_mt_100[FH2O_ckd_mt_100_npt+addF77fields]

Definition at line 2661 of file continua.h.

Referenced by CKD_mt_100_foreign_h2o().

const Numeric FH2O_ckd_mt_100_dv = 10.0

Definition at line 2659 of file continua.h.

Referenced by CKD_mt_100_foreign_h2o().

const int FH2O_ckd_mt_100_npt = 2003

Definition at line 2660 of file continua.h.

Referenced by CKD_mt_100_foreign_h2o().

const Numeric FH2O_ckd_mt_100_v1 = -20.0

Definition at line 2657 of file continua.h.

Referenced by CKD_mt_100_foreign_h2o().

const Numeric FH2O_ckd_mt_100_v2 = 20000.0

Definition at line 2658 of file continua.h.

Referenced by CKD_mt_100_foreign_h2o().

const double N2N2_CT220_ckd_mt_100[N2N2_CT220_ckd_mt_100_npt+addF77fields]

Initial value:

 {
           0.0000e0,
           0.4946E-06, 0.5756E-06, 0.5964E-06, 0.5756E-06, 0.4946E-06,
           0.4145E-06, 0.3641E-06, 0.3482E-06, 0.3340E-06, 0.3252E-06,
           0.3299E-06, 0.3206E-06, 0.3184E-06, 0.3167E-06, 0.2994E-06,
           0.2943E-06, 0.2794E-06, 0.2582E-06, 0.2468E-06, 0.2237E-06,
           0.2038E-06, 0.1873E-06, 0.1641E-06, 0.1474E-06, 0.1297E-06,
           0.1114E-06, 0.9813E-07, 0.8309E-07, 0.7059E-07, 0.6068E-07,
           0.5008E-07, 0.4221E-07, 0.3537E-07, 0.2885E-07, 0.2407E-07,
           0.1977E-07, 0.1605E-07, 0.1313E-07, 0.1057E-07, 0.8482E-08,
           0.6844E-08, 0.5595E-08, 0.4616E-08, 0.3854E-08, 0.3257E-08,
           0.2757E-08, 0.2372E-08, 0.2039E-08, 0.1767E-08, 0.1548E-08,
           0.1346E-08, 0.1181E-08, 0.1043E-08, 0.9110E-09, 0.8103E-09,
           0.7189E-09, 0.6314E-09, 0.5635E-09, 0.4976E-09, 0.4401E-09,
           0.3926E-09, 0.3477E-09, 0.3085E-09, 0.2745E-09, 0.2416E-09,
           0.2155E-09, 0.1895E-09, 0.1678E-09, 0.1493E-09, 0.1310E-09,
           0.1154E-09, 0.1019E-09, 0.8855E-10}

Definition at line 3317 of file continua.h.

Referenced by CKD_mt_CIArot_n2().

const Numeric N2N2_CT220_ckd_mt_100_dv = 5.0

Definition at line 3315 of file continua.h.

Referenced by CKD_mt_CIArot_n2().

const int N2N2_CT220_ckd_mt_100_npt = 73

Definition at line 3316 of file continua.h.

Referenced by CKD_mt_CIArot_n2().

const Numeric N2N2_CT220_ckd_mt_100_v1 = -10.0

Definition at line 3313 of file continua.h.

Referenced by CKD_mt_CIArot_n2().

const Numeric N2N2_CT220_ckd_mt_100_v2 = 350.0

Definition at line 3314 of file continua.h.

Referenced by CKD_mt_CIArot_n2().

const double N2N2_CT296_ckd_mt_100[N2N2_CT296_ckd_mt_100_npt+addF77fields]

Initial value:

 {
           0.0000e0, 
           0.4303E-06, 0.4850E-06, 0.4979E-06, 0.4850E-06, 0.4303E-06,
           0.3715E-06, 0.3292E-06, 0.3086E-06, 0.2920E-06, 0.2813E-06,
           0.2804E-06, 0.2738E-06, 0.2726E-06, 0.2724E-06, 0.2635E-06,
           0.2621E-06, 0.2547E-06, 0.2428E-06, 0.2371E-06, 0.2228E-06,
           0.2100E-06, 0.1991E-06, 0.1822E-06, 0.1697E-06, 0.1555E-06,
           0.1398E-06, 0.1281E-06, 0.1138E-06, 0.1012E-06, 0.9078E-07,
           0.7879E-07, 0.6944E-07, 0.6084E-07, 0.5207E-07, 0.4540E-07,
           0.3897E-07, 0.3313E-07, 0.2852E-07, 0.2413E-07, 0.2045E-07,
           0.1737E-07, 0.1458E-07, 0.1231E-07, 0.1031E-07, 0.8586E-08,
           0.7162E-08, 0.5963E-08, 0.4999E-08, 0.4226E-08, 0.3607E-08,
           0.3090E-08, 0.2669E-08, 0.2325E-08, 0.2024E-08, 0.1783E-08,
           0.1574E-08, 0.1387E-08, 0.1236E-08, 0.1098E-08, 0.9777E-09,
           0.8765E-09, 0.7833E-09, 0.7022E-09, 0.6317E-09, 0.5650E-09,
           0.5100E-09, 0.4572E-09, 0.4115E-09, 0.3721E-09, 0.3339E-09,
           0.3005E-09, 0.2715E-09, 0.2428E-09}

Definition at line 3287 of file continua.h.

Referenced by CKD_mt_CIArot_n2().

const Numeric N2N2_CT296_ckd_mt_100_dv = 5.0

Definition at line 3285 of file continua.h.

Referenced by CKD_mt_CIArot_n2().

const int N2N2_CT296_ckd_mt_100_npt = 73

Definition at line 3286 of file continua.h.

Referenced by CKD_mt_CIArot_n2().

const Numeric N2N2_CT296_ckd_mt_100_v1 = -10.0

Definition at line 3283 of file continua.h.

Referenced by CKD_mt_CIArot_n2().

const Numeric N2N2_CT296_ckd_mt_100_v2 = 350.0

Definition at line 3284 of file continua.h.

Referenced by CKD_mt_CIArot_n2().

const double N2N2_N2F_ckd_mt_100[N2N2_N2F_ckd_mt_100_npt+addF77fields]

Initial value:

 {
            0.000E+00, 
            0.000E+00,  2.000E-10,  5.200E-09,  1.020E-08,  1.520E-08,  
            2.020E-08,  2.520E-08,  3.020E-08,  4.450E-08,  5.220E-08,  
            6.460E-08,  7.750E-08,  9.030E-08,  1.060E-07,  1.210E-07,  
            1.370E-07,  1.570E-07,  1.750E-07,  2.010E-07,  2.300E-07,  
            2.590E-07,  2.950E-07,  3.260E-07,  3.660E-07,  4.050E-07,  
            4.470E-07,  4.920E-07,  5.340E-07,  5.840E-07,  6.240E-07,  
            6.670E-07,  7.140E-07,  7.260E-07,  7.540E-07,  7.840E-07,  
            8.090E-07,  8.420E-07,  8.620E-07,  8.870E-07,  9.110E-07,  
            9.360E-07,  9.760E-07,  1.030E-06,  1.110E-06,  1.230E-06,  
            1.390E-06,  1.610E-06,  1.760E-06,  1.940E-06,  1.970E-06,  
            1.870E-06,  1.750E-06,  1.560E-06,  1.420E-06,  1.350E-06,  
            1.320E-06,  1.290E-06,  1.290E-06,  1.290E-06,  1.300E-06,  
            1.320E-06,  1.330E-06,  1.340E-06,  1.350E-06,  1.330E-06,  
            1.310E-06,  1.290E-06,  1.240E-06,  1.200E-06,  1.160E-06,  
            1.100E-06,  1.040E-06,  9.960E-07,  9.380E-07,  8.630E-07,  
            7.980E-07,  7.260E-07,  6.550E-07,  5.940E-07,  5.350E-07,  
            4.740E-07,  4.240E-07,  3.770E-07,  3.330E-07,  2.960E-07,  
            2.630E-07,  2.340E-07,  2.080E-07,  1.850E-07,  1.670E-07,  
            1.470E-07,  1.320E-07,  1.200E-07,  1.090E-07,  9.850E-08,  
            9.080E-08,  8.180E-08,  7.560E-08,  6.850E-08,  6.140E-08,  
            5.830E-08,  5.770E-08,  5.000E-08,  4.320E-08,  3.140E-08,  
            2.890E-08,  2.640E-08,  2.390E-08,  2.140E-08,  1.890E-08,  
            1.640E-08,  1.390E-08,  1.140E-08,  8.900E-09,  6.400E-09,  
            3.900E-09,  1.400E-09,  0.000E+00}

Definition at line 3345 of file continua.h.

Referenced by CKD_mt_CIAfun_n2().

const Numeric N2N2_N2F_ckd_mt_100_dv = 5.000

Definition at line 3343 of file continua.h.

Referenced by CKD_mt_CIAfun_n2().

const int N2N2_N2F_ckd_mt_100_npt = 118

Definition at line 3344 of file continua.h.

Referenced by CKD_mt_CIAfun_n2().

const Numeric N2N2_N2F_ckd_mt_100_v1 = 2085.000

Definition at line 3341 of file continua.h.

Referenced by CKD_mt_CIAfun_n2().

const Numeric N2N2_N2F_ckd_mt_100_v2 = 2670.000

Definition at line 3342 of file continua.h.

Referenced by CKD_mt_CIAfun_n2().

const double N2N2_N2Ft_ckd_mt_100[N2N2_N2F_ckd_mt_100_npt+addF77fields]

Initial value:

 {
            0.000E+00, 
            1.040E+03,  1.010E+03,  9.800E+02,  9.500E+02,  9.200E+02,  
            8.900E+02,  8.600E+02,  8.300E+02,  8.020E+02,  7.610E+02,  
            7.220E+02,  6.790E+02,  6.460E+02,  6.090E+02,  5.620E+02,  
            5.110E+02,  4.720E+02,  4.360E+02,  4.060E+02,  3.770E+02,  
            3.550E+02,  3.380E+02,  3.190E+02,  2.990E+02,  2.780E+02,  
            2.550E+02,  2.330E+02,  2.080E+02,  1.840E+02,  1.490E+02,  
            1.070E+02,  6.600E+01,  2.500E+01, -1.300E+01, -4.900E+01,  
           -8.200E+01, -1.040E+02, -1.190E+02, -1.300E+02, -1.390E+02,  
           -1.440E+02, -1.460E+02, -1.460E+02, -1.470E+02, -1.480E+02,  
           -1.500E+02, -1.530E+02, -1.600E+02, -1.690E+02, -1.810E+02,  
           -1.890E+02, -1.950E+02, -2.000E+02, -2.050E+02, -2.090E+02,  
           -2.110E+02, -2.100E+02, -2.100E+02, -2.090E+02, -2.050E+02,  
           -1.990E+02, -1.900E+02, -1.800E+02, -1.680E+02, -1.570E+02,  
           -1.430E+02, -1.260E+02, -1.080E+02, -8.900E+01, -6.300E+01,  
           -3.200E+01,  1.000E+00,  3.500E+01,  6.500E+01,  9.500E+01,  
            1.210E+02,  1.410E+02,  1.520E+02,  1.610E+02,  1.640E+02,  
            1.640E+02,  1.610E+02,  1.550E+02,  1.480E+02,  1.430E+02,  
            1.370E+02,  1.330E+02,  1.310E+02,  1.330E+02,  1.390E+02,  
            1.500E+02,  1.650E+02,  1.870E+02,  2.130E+02,  2.480E+02,  
            2.840E+02,  3.210E+02,  3.720E+02,  4.490E+02,  5.140E+02,  
            5.690E+02,  6.090E+02,  6.420E+02,  6.730E+02,  7.000E+02,  
            7.300E+02,  7.600E+02,  7.900E+02,  8.200E+02,  8.500E+02,  
            8.800E+02,  9.100E+02,  9.400E+02,  9.700E+02,  1.000E+03,  
            1.030E+03,  1.060E+03,  1.090E+03}

Definition at line 3373 of file continua.h.

Referenced by CKD_mt_CIAfun_n2().

const double O2_00_ckd_mt_100[O2_00_ckd_mt_100_npt+addF77fields]

Definition at line 3480 of file continua.h.

Referenced by CKD_mt_v0v0_o2().

const Numeric O2_00_ckd_mt_100_dv = 2.000e0

Definition at line 3478 of file continua.h.

Referenced by CKD_mt_v0v0_o2().

const int O2_00_ckd_mt_100_npt = 483

Definition at line 3479 of file continua.h.

Referenced by CKD_mt_v0v0_o2().

const Numeric O2_00_ckd_mt_100_v1 = 7536.000e0

Definition at line 3476 of file continua.h.

Referenced by CKD_mt_v0v0_o2().

const Numeric O2_00_ckd_mt_100_v2 = 8500.000e0

Definition at line 3477 of file continua.h.

Referenced by CKD_mt_v0v0_o2().

const Numeric O2_10_ckd_mt_100_dv = 2.000e0

Definition at line 3597 of file continua.h.

Referenced by CKD_mt_v1v0_o2().

const Numeric O2_10_ckd_mt_100_v1 = 9100.000e0

Definition at line 3595 of file continua.h.

Referenced by CKD_mt_v1v0_o2().

const Numeric O2_10_ckd_mt_100_v2 = 11000.000e0

Definition at line 3596 of file continua.h.

Referenced by CKD_mt_v1v0_o2().

const Numeric O2O2_O2F_ckd_mt_100_dv = 5.000

Definition at line 3409 of file continua.h.

Referenced by CKD_mt_CIAfun_o2().

const int O2O2_O2F_ckd_mt_100_npt = 103

Definition at line 3410 of file continua.h.

Referenced by CKD_mt_CIAfun_o2().

const Numeric O2O2_O2F_ckd_mt_100_v1 = 1340.000

Definition at line 3407 of file continua.h.

Referenced by CKD_mt_CIAfun_o2().

const Numeric O2O2_O2F_ckd_mt_100_v2 = 1850.000

Definition at line 3408 of file continua.h.

Referenced by CKD_mt_CIAfun_o2().

const double O2O2_O2Fo_ckd_mt_100[O2O2_O2F_ckd_mt_100_npt+addF77fields]

Initial value:

 {
            0.000E+00, 
            0.000E+00,  9.744E-09,  2.256E-08,  3.538E-08,  4.820E-08,  
            6.100E-08,  7.400E-08,  8.400E-08,  9.600E-08,  1.200E-07,  
            1.620E-07,  2.080E-07,  2.460E-07,  2.850E-07,  3.140E-07,  
            3.800E-07,  4.440E-07,  5.000E-07,  5.710E-07,  6.730E-07,  
            7.680E-07,  8.530E-07,  9.660E-07,  1.100E-06,  1.210E-06,  
            1.330E-06,  1.470E-06,  1.590E-06,  1.690E-06,  1.800E-06,  
            1.920E-06,  2.040E-06,  2.150E-06,  2.260E-06,  2.370E-06,  
            2.510E-06,  2.670E-06,  2.850E-06,  3.070E-06,  3.420E-06,  
            3.830E-06,  4.200E-06,  4.450E-06,  4.600E-06,  4.530E-06,  
            4.280E-06,  3.960E-06,  3.680E-06,  3.480E-06,  3.350E-06,  
            3.290E-06,  3.250E-06,  3.230E-06,  3.230E-06,  3.210E-06,  
            3.190E-06,  3.110E-06,  3.030E-06,  2.910E-06,  2.800E-06,  
            2.650E-06,  2.510E-06,  2.320E-06,  2.130E-06,  1.930E-06,  
            1.760E-06,  1.590E-06,  1.420E-06,  1.250E-06,  1.110E-06,  
            9.900E-07,  8.880E-07,  7.910E-07,  6.780E-07,  5.870E-07,  
            5.240E-07,  4.640E-07,  4.030E-07,  3.570E-07,  3.200E-07,  
            2.900E-07,  2.670E-07,  2.420E-07,  2.150E-07,  1.820E-07,  
            1.600E-07,  1.460E-07,  1.280E-07,  1.030E-07,  8.700E-08,  
            8.100E-08,  7.100E-08,  6.400E-08,  5.807E-08,  5.139E-08,  
            4.496E-08,  3.854E-08,  3.212E-08,  2.569E-08,  1.927E-08,  
            1.285E-08,  6.423E-09,  0.000E+00}

Definition at line 3411 of file continua.h.

Referenced by CKD_mt_CIAfun_o2().

const double O2O2_O2Ft_ckd_mt_100[O2O2_O2F_ckd_mt_100_npt+addF77fields]

Initial value:

 {
            0.000E+00, 
            4.000E+02,  4.000E+02,  4.000E+02,  4.000E+02,  4.000E+02,  
            4.670E+02,  4.000E+02,  3.150E+02,  3.790E+02,  3.680E+02,  
            4.750E+02,  5.210E+02,  5.310E+02,  5.120E+02,  4.420E+02,  
            4.440E+02,  4.300E+02,  3.810E+02,  3.350E+02,  3.240E+02,  
            2.960E+02,  2.480E+02,  2.150E+02,  1.930E+02,  1.580E+02,  
            1.270E+02,  1.010E+02,  7.100E+01,  3.100E+01, -6.000E+00,  
           -2.600E+01, -4.700E+01, -6.300E+01, -7.900E+01, -8.800E+01,  
           -8.800E+01, -8.700E+01, -9.000E+01, -9.800E+01, -9.900E+01,  
           -1.090E+02, -1.340E+02, -1.600E+02, -1.670E+02, -1.640E+02,  
           -1.580E+02, -1.530E+02, -1.510E+02, -1.560E+02, -1.660E+02,  
           -1.680E+02, -1.730E+02, -1.700E+02, -1.610E+02, -1.450E+02,  
           -1.260E+02, -1.080E+02, -8.400E+01, -5.900E+01, -2.900E+01,  
            4.000E+00,  4.100E+01,  7.300E+01,  9.700E+01,  1.230E+02,  
            1.590E+02,  1.980E+02,  2.200E+02,  2.420E+02,  2.560E+02,  
            2.810E+02,  3.110E+02,  3.340E+02,  3.190E+02,  3.130E+02,  
            3.210E+02,  3.230E+02,  3.100E+02,  3.150E+02,  3.200E+02,  
            3.350E+02,  3.610E+02,  3.780E+02,  3.730E+02,  3.380E+02,  
            3.190E+02,  3.460E+02,  3.220E+02,  2.910E+02,  2.900E+02,  
            3.500E+02,  3.710E+02,  5.040E+02,  4.000E+02,  4.000E+02,  
            4.000E+02,  4.000E+02,  4.000E+02,  4.000E+02,  4.000E+02,  
            4.000E+02,  4.000E+02,  4.000E+02}

Definition at line 3435 of file continua.h.

Referenced by CKD_mt_CIAfun_o2().

const double SL260_ckd_0[SL260_ckd_0_npt+addF77fields]

Definition at line 1391 of file continua.h.

Referenced by CKD_222_self_h2o(), and CKD_242_self_h2o().

const Numeric SL260_ckd_0_dv = 10.0

Definition at line 1389 of file continua.h.

Referenced by CKD_222_self_h2o(), and CKD_242_self_h2o().

const int SL260_ckd_0_npt = 2003

Definition at line 1390 of file continua.h.

Referenced by CKD_222_self_h2o(), and CKD_242_self_h2o().

const Numeric SL260_ckd_0_v1 = -20.0

Definition at line 1387 of file continua.h.

Referenced by CKD_222_self_h2o(), and CKD_242_self_h2o().

const Numeric SL260_ckd_0_v2 = 20000.0

Definition at line 1388 of file continua.h.

Referenced by CKD_222_self_h2o(), and CKD_242_self_h2o().

const double SL260_ckd_mt_100[SL260_ckd_mt_100_npt+addF77fields]

Definition at line 2249 of file continua.h.

Referenced by CKD_mt_100_self_h2o().

const Numeric SL260_ckd_mt_100_dv = 10.0

Definition at line 2247 of file continua.h.

Referenced by CKD_mt_100_self_h2o().

const int SL260_ckd_mt_100_npt = 2003

Definition at line 2248 of file continua.h.

Referenced by CKD_mt_100_self_h2o().

const Numeric SL260_ckd_mt_100_v1 = -20.0

Definition at line 2245 of file continua.h.

Referenced by CKD_mt_100_self_h2o().

const Numeric SL260_ckd_mt_100_v2 = 20000.0

Definition at line 2246 of file continua.h.

Referenced by CKD_mt_100_self_h2o().

const double SL296_ckd_0[SL296_ckd_0_npt+addF77fields]

Definition at line 562 of file continua.h.

Referenced by CKD_222_self_h2o(), and CKD_242_self_h2o().

const Numeric SL296_ckd_0_dv = 10.0

Definition at line 560 of file continua.h.

Referenced by CKD_222_self_h2o(), and CKD_242_self_h2o().

const int SL296_ckd_0_npt = 2003

Definition at line 561 of file continua.h.

Referenced by CKD_222_self_h2o(), and CKD_242_self_h2o().

const Numeric SL296_ckd_0_v1 = -20.0

Definition at line 558 of file continua.h.

Referenced by CKD_222_self_h2o(), and CKD_242_self_h2o().

const Numeric SL296_ckd_0_v2 = 20000.0

Definition at line 559 of file continua.h.

Referenced by CKD_222_self_h2o(), and CKD_242_self_h2o().

const double SL296_ckd_mt_100[SL296_ckd_mt_100_npt+addF77fields]

Definition at line 1838 of file continua.h.

Referenced by CKD_mt_100_self_h2o().

const Numeric SL296_ckd_mt_100_dv = 10.0

Definition at line 1836 of file continua.h.

Referenced by CKD_mt_100_self_h2o().

const int SL296_ckd_mt_100_npt = 2003

Definition at line 1837 of file continua.h.

Referenced by CKD_mt_100_self_h2o().

const Numeric SL296_ckd_mt_100_v1 = -20.0

Definition at line 1834 of file continua.h.

Referenced by CKD_mt_100_self_h2o().

const Numeric SL296_ckd_mt_100_v2 = 20000.0

Definition at line 1835 of file continua.h.

Referenced by CKD_mt_100_self_h2o().


Functions
void	xsec_continuum_tag (MatrixView xsec, const String &name, ConstVectorView parameters, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView abs_n2, ConstVectorView abs_h2o, ConstVectorView vmr)
	Calculates model absorption for one continuum or full model tag.
void	check_continuum_model (const String &name)
	An auxiliary functions that checks if a given continuum model is listed in species_data.cc.
void	MPM87H2OAbsModel (MatrixView xsec, const Numeric CC, const Numeric CL, const Numeric CW, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	MPM87H2OAbsModel.
void	MPM89H2OAbsModel (MatrixView xsec, const Numeric CCin, const Numeric CLin, const Numeric CWin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	MPM89H2OAbsModel.
void	MPM93H2OAbsModel (MatrixView xsec, const Numeric CCin, const Numeric CLin, const Numeric CWin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	MPM93H2OAbsModel.
void	PWR98H2OAbsModel (MatrixView xsec, const Numeric CCin, const Numeric CLin, const Numeric CWin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	PWR98H2OAbsModel.
void	CP98H2OAbsModel (MatrixView xsec, const Numeric CCin, const Numeric CLin, const Numeric CWin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	CP98H2OAbsModel.
void	Pardo_ATM_H2O_ForeignContinuum (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	Pardo_ATM_H2O_ForeignContinuum.
void	Standard_H2O_self_continuum (MatrixView xsec, const Numeric C, const Numeric x, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	Standard_H2O_self_continuum.
void	Standard_H2O_foreign_continuum (MatrixView xsec, const Numeric C, const Numeric x, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	Standard_H2O_foreign_continuum.
void	MaTipping_H2O_foreign_continuum (MatrixView xsec, const Numeric C, const Numeric x, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	MaTipping_H2O_foreign_continuum.
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_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	MPM93 H2O pseudo continuum line parameters:.
void	CKD_222_self_h2o (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr, ConstVectorView abs_n2)
	CKD version 2.2.2 H2O self continuum absorption model.
void	CKD_222_foreign_h2o (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr, ConstVectorView abs_n2)
	CKD version 2.2.2 H2O foreign continuum absorption model.
void	CKD_242_self_h2o (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr, ConstVectorView abs_n2)
	CKD version 2.4.2 H2O self continuum absorption model.
void	CKD24_H20 (MatrixView xsec, int isf, const Numeric Cin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr, ConstVectorView abs_n2)
	CKD version 2.4 H2O continuum absorption model.
void	CKD_242_foreign_h2o (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr, ConstVectorView abs_n2)
	CKD version 2.4.2 H2O foreign continuum absorption model.
void	CKD_mt_100_self_h2o (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr, ConstVectorView abs_n2)
	CKD version MT 1.00 H2O self continuum absorption model.
void	CKD_mt_100_foreign_h2o (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr, ConstVectorView abs_n2)
	CKD version MT 1.00 H2O foreign continuum absorption model.
void	MPM85O2AbsModel (MatrixView xsec, const Numeric CC, const Numeric CL, const Numeric CW, const Numeric CO, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView abs_h2o, ConstVectorView vmr)
	MPM85O2AbsModel.
void	MPM87O2AbsModel (MatrixView xsec, const Numeric CC, const Numeric CL, const Numeric CW, const Numeric CO, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView abs_h2o, ConstVectorView vmr)
	MPM87O2AbsModel.
void	MPM89O2AbsModel (MatrixView xsec, const Numeric CC, const Numeric CL, const Numeric CW, const Numeric CO, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView abs_h2o, ConstVectorView vmr)
	MPM89O2AbsModel.
void	MPM92O2AbsModel (MatrixView xsec, const Numeric CC, const Numeric CL, const Numeric CW, const Numeric CO, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView abs_h2o, ConstVectorView vmr)
	MPM92O2AbsModel.
void	MPM93O2AbsModel (MatrixView xsec, const Numeric CC, const Numeric CL, const Numeric CW, const Numeric CO, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView abs_h2o, ConstVectorView vmr)
	MPM93O2AbsModel.
void	PWR93O2AbsModel (MatrixView xsec, const Numeric CC, const Numeric CL, const Numeric CW, const Numeric CO, const String &model, const String &version, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView abs_h2o, ConstVectorView vmr)
	Oxygen complex at 60 GHz plus mm O2 lines plus O2 continuum.
void	MPM93_O2_continuum (MatrixView xsec, const Numeric S0in, const Numeric G0in, const Numeric XSOin, const Numeric XG0in, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView abs_h2o, ConstVectorView vmr)
	MPM93 O2 continuum:.
void	Rosenkranz_O2_continuum (MatrixView xsec, const Numeric S0in, const Numeric G0in, const Numeric XSOin, const Numeric XG0in, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView abs_h2o, ConstVectorView vmr)
	3) O2-air
void	CKD_mt_CIAfun_o2 (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	CKD version MT 1.00 O2-O2 collision induced absorption (fundamental band).
void	CKD_mt_v0v0_o2 (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr, ConstVectorView abs_n2)
	CKD version MT 1.00 O2 v0<-v0 band absorption.
void	CKD_mt_v1v0_o2 (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	CKD version MT 1.00 O2 v1<-v0 band absorption.
void	CKD_mt_CIArot_n2 (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	CKD version MT 1.00 N2-N2 collision induced absorption (rotational band).
void	CKD_mt_CIAfun_n2 (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	CKD version MT 1.00 N2-N2 collision induced absorption (fundamental band).
void	BF86_CIA_N2 (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	Borysow-Frommhold 1986 N2-N2 CIA absorption model;.
void	MPM93_N2_continuum (MatrixView xsec, const Numeric Cin, const Numeric Gin, const Numeric xTin, const Numeric xfin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView abs_h2o, ConstVectorView vmr)
	MPM93 N2 continuum.
void	Rosenkranz_N2_self_continuum (MatrixView xsec, const Numeric Cin, const Numeric xin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	Rosenkranz_N2_self_continuum.
void	Standard_N2_self_continuum (MatrixView xsec, const Numeric Cin, const Numeric xfin, const Numeric xtin, const Numeric xpin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	4) N2-N2
void	Pardo_ATM_N2_dry_continuum (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr, ConstVectorView abs_h2o)
	Pardo_ATM_N2_dry_continuum.
void	CKD_241_co2 (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	CKD version 2.4.1 CO2 continuum absorption model.
void	CKD_mt_co2 (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	CKD version MT 1.00 CO2 continuum absorption model.
void	Rosenkranz_CO2_self_continuum (MatrixView xsec, const Numeric C, const Numeric x, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	Rosenkranz_CO2_self_continuum.
void	Rosenkranz_CO2_foreign_continuum (MatrixView xsec, const Numeric C, const Numeric x, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView abs_n2, ConstVectorView vmr)
	Rosenkranz_CO2_foreign_continuum.
void	MPM93WaterDropletAbs (MatrixView xsec, const Numeric CC, const Numeric CG, const Numeric CE, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	MPM93WaterDropletAbs.
void	MPM93IceCrystalAbs (MatrixView xsec, const Numeric CC, const Numeric CA, const Numeric CB, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	MPM93IceCrystalAbs.
void	MPM93RainExt (MatrixView xsec, const Numeric CE, const Numeric CA, const Numeric CB, const String &model, ConstVectorView f_grid, ConstVectorView abs_p, ConstVectorView abs_t, ConstVectorView vmr)
	MPM93RainExt.
Numeric	MPMLineShapeFunction (const Numeric gamma, const Numeric fl, const Numeric f)
Numeric	MPMLineShapeO2Function (const Numeric gamma, const Numeric fl, const Numeric f, const Numeric delta)
Numeric	WVSatPressureLiquidWater (const Numeric t)
Numeric	WVSatPressureIce (const Numeric t)
Variables
const int	addF77fields = 1
const Numeric	SL296_ckd_0_v1 = -20.0
const Numeric	SL296_ckd_0_v2 = 20000.0
const Numeric	SL296_ckd_0_dv = 10.0
const int	SL296_ckd_0_npt = 2003
const double	SL296_ckd_0 [SL296_ckd_0_npt+addF77fields]
const Numeric	FH2O_ckd_0_v1 = -20.0
const Numeric	FH2O_ckd_0_v2 = 20000.0
const Numeric	FH2O_ckd_0_dv = 10.0
const int	FH2O_ckd_0_npt = 2003
const double	FH2O_ckd_0 [FH2O_ckd_0_npt+addF77fields]
const Numeric	SL260_ckd_0_v1 = -20.0
const Numeric	SL260_ckd_0_v2 = 20000.0
const Numeric	SL260_ckd_0_dv = 10.0
const int	SL260_ckd_0_npt = 2003
const double	SL260_ckd_0 [SL260_ckd_0_npt+addF77fields]
const Numeric	SL296_ckd_mt_100_v1 = -20.0
const Numeric	SL296_ckd_mt_100_v2 = 20000.0
const Numeric	SL296_ckd_mt_100_dv = 10.0
const int	SL296_ckd_mt_100_npt = 2003
const double	SL296_ckd_mt_100 [SL296_ckd_mt_100_npt+addF77fields]
const Numeric	SL260_ckd_mt_100_v1 = -20.0
const Numeric	SL260_ckd_mt_100_v2 = 20000.0
const Numeric	SL260_ckd_mt_100_dv = 10.0
const int	SL260_ckd_mt_100_npt = 2003
const double	SL260_ckd_mt_100 [SL260_ckd_mt_100_npt+addF77fields]
const Numeric	FH2O_ckd_mt_100_v1 = -20.0
const Numeric	FH2O_ckd_mt_100_v2 = 20000.0
const Numeric	FH2O_ckd_mt_100_dv = 10.0
const int	FH2O_ckd_mt_100_npt = 2003
const double	FH2O_ckd_mt_100 [FH2O_ckd_mt_100_npt+addF77fields]
const Numeric	FCO2_ckd_mt_100_v1 = -20.0
const Numeric	FCO2_ckd_mt_100_v2 = 10000.0
const Numeric	FCO2_ckd_mt_100_dv = 10.0
const int	FCO2_ckd_mt_100_npt = 1003
const double	FCO2_ckd_mt_100 [FCO2_ckd_mt_100_npt+addF77fields]
const Numeric	N2N2_CT296_ckd_mt_100_v1 = -10.0
const Numeric	N2N2_CT296_ckd_mt_100_v2 = 350.0
const Numeric	N2N2_CT296_ckd_mt_100_dv = 5.0
const int	N2N2_CT296_ckd_mt_100_npt = 73
const double	N2N2_CT296_ckd_mt_100 [N2N2_CT296_ckd_mt_100_npt+addF77fields]
const Numeric	N2N2_CT220_ckd_mt_100_v1 = -10.0
const Numeric	N2N2_CT220_ckd_mt_100_v2 = 350.0
const Numeric	N2N2_CT220_ckd_mt_100_dv = 5.0
const int	N2N2_CT220_ckd_mt_100_npt = 73
const double	N2N2_CT220_ckd_mt_100 [N2N2_CT220_ckd_mt_100_npt+addF77fields]
const Numeric	N2N2_N2F_ckd_mt_100_v1 = 2085.000
const Numeric	N2N2_N2F_ckd_mt_100_v2 = 2670.000
const Numeric	N2N2_N2F_ckd_mt_100_dv = 5.000
const int	N2N2_N2F_ckd_mt_100_npt = 118
const double	N2N2_N2F_ckd_mt_100 [N2N2_N2F_ckd_mt_100_npt+addF77fields]
const double	N2N2_N2Ft_ckd_mt_100 [N2N2_N2F_ckd_mt_100_npt+addF77fields]
const Numeric	O2O2_O2F_ckd_mt_100_v1 = 1340.000
const Numeric	O2O2_O2F_ckd_mt_100_v2 = 1850.000
const Numeric	O2O2_O2F_ckd_mt_100_dv = 5.000
const int	O2O2_O2F_ckd_mt_100_npt = 103
const double	O2O2_O2Fo_ckd_mt_100 [O2O2_O2F_ckd_mt_100_npt+addF77fields]
const double	O2O2_O2Ft_ckd_mt_100 [O2O2_O2F_ckd_mt_100_npt+addF77fields]
const Numeric	O2_00_ckd_mt_100_v1 = 7536.000e0
const Numeric	O2_00_ckd_mt_100_v2 = 8500.000e0
const Numeric	O2_00_ckd_mt_100_dv = 2.000e0
const int	O2_00_ckd_mt_100_npt = 483
const double	O2_00_ckd_mt_100 [O2_00_ckd_mt_100_npt+addF77fields]
const Numeric	O2_10_ckd_mt_100_v1 = 9100.000e0
const Numeric	O2_10_ckd_mt_100_v2 = 11000.000e0
const Numeric	O2_10_ckd_mt_100_dv = 2.000e0

continua.h File Reference

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