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

#include "matpackI.h"

Functions
void	xsec_continuum_tag (MatrixView xsec, const String &name, ConstVectorView parameters, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView n2_abs, ConstVectorView h2o_abs, ConstVectorView vmr)
	Calculates model absorption for one continuum or full model tag. More...

void	check_continuum_model (const String &name)
	An auxiliary functions that checks if a given continuum model is listed in species_data.cc. More...

void	MPM87H2OAbsModel (MatrixView xsec, const Numeric CC, const Numeric CL, const Numeric CW, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

void	MPM89H2OAbsModel (MatrixView xsec, const Numeric CCin, const Numeric CLin, const Numeric CWin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

void	MPM93H2OAbsModel (MatrixView xsec, const Numeric CCin, const Numeric CLin, const Numeric CWin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

void	PWR98H2OAbsModel (MatrixView xsec, const Numeric CCin, const Numeric CLin, const Numeric CWin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

void	CP98H2OAbsModel (MatrixView xsec, const Numeric CCin, const Numeric CLin, const Numeric CWin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

void	Pardo_ATM_H2O_ForeignContinuum (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

void	Standard_H2O_self_continuum (MatrixView xsec, const Numeric C, const Numeric x, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

void	Standard_H2O_foreign_continuum (MatrixView xsec, const Numeric C, const Numeric x, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

void	MaTipping_H2O_foreign_continuum (MatrixView xsec, const Numeric C, const Numeric x, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

void	MPM93_H2O_continuum (MatrixView xsec, const Numeric fcenter, const Numeric b1, const Numeric b2, const Numeric b3, const Numeric b4, const Numeric b5, const Numeric b6, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

void	CKD_222_self_h2o (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr, ConstVectorView n2_abs)

void	CKD_222_foreign_h2o (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr, ConstVectorView n2_abs)

void	CKD_242_self_h2o (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr, ConstVectorView n2_abs)

void	CKD24_H20 (MatrixView xsec, int isf, const Numeric Cin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr, ConstVectorView n2_abs)

void	CKD_242_foreign_h2o (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr, ConstVectorView n2_abs)

void	CKD_mt_100_self_h2o (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr, ConstVectorView n2_abs)

void	CKD_mt_100_foreign_h2o (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr, ConstVectorView n2_abs)

void	MPM85O2AbsModel (MatrixView xsec, const Numeric CC, const Numeric CL, const Numeric CW, const Numeric CO, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView h2o_abs, ConstVectorView vmr)

void	MPM87O2AbsModel (MatrixView xsec, const Numeric CC, const Numeric CL, const Numeric CW, const Numeric CO, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView h2o_abs, ConstVectorView vmr)

void	MPM89O2AbsModel (MatrixView xsec, const Numeric CC, const Numeric CL, const Numeric CW, const Numeric CO, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView h2o_abs, ConstVectorView vmr)

void	MPM92O2AbsModel (MatrixView xsec, const Numeric CC, const Numeric CL, const Numeric CW, const Numeric CO, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView h2o_abs, ConstVectorView vmr)

void	MPM93O2AbsModel (MatrixView xsec, const Numeric CC, const Numeric CL, const Numeric CW, const Numeric CO, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView h2o_abs, ConstVectorView vmr)

void	PWR93O2AbsModel (MatrixView xsec, const Numeric CC, const Numeric CL, const Numeric CW, const Numeric CO, const String &model, const String &version, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView h2o_abs, ConstVectorView vmr)

void	MPM93_O2_continuum (MatrixView xsec, const Numeric S0in, const Numeric G0in, const Numeric XSOin, const Numeric XG0in, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView h2o_abs, ConstVectorView vmr)

void	Rosenkranz_O2_continuum (MatrixView xsec, const Numeric S0in, const Numeric G0in, const Numeric XSOin, const Numeric XG0in, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView h2o_abs, ConstVectorView vmr)

void	CKD_mt_CIAfun_o2 (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

void	CKD_mt_v0v0_o2 (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr, ConstVectorView n2_abs)

void	CKD_mt_v1v0_o2 (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

void	CKD_mt_CIArot_n2 (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

void	CKD_mt_CIAfun_n2 (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

void	BF86_CIA_N2 (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

void	MPM93_N2_continuum (MatrixView xsec, const Numeric Cin, const Numeric Gin, const Numeric xTin, const Numeric xfin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView h2o_abs, ConstVectorView vmr)

void	Rosenkranz_N2_self_continuum (MatrixView xsec, const Numeric Cin, const Numeric xin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

void	Standard_N2_self_continuum (MatrixView xsec, const Numeric Cin, const Numeric xfin, const Numeric xtin, const Numeric xpin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

void	Pardo_ATM_N2_dry_continuum (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr, ConstVectorView h2o_abs)

void	CKD_241_co2 (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

void	CKD_mt_co2 (MatrixView xsec, const Numeric Cin, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

void	Rosenkranz_CO2_self_continuum (MatrixView xsec, const Numeric C, const Numeric x, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

void	Rosenkranz_CO2_foreign_continuum (MatrixView xsec, const Numeric C, const Numeric x, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView n2_abs, ConstVectorView vmr)

void	MPM93WaterDropletAbs (MatrixView xsec, const Numeric CC, const Numeric CG, const Numeric CE, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

void	MPM93IceCrystalAbs (MatrixView xsec, const Numeric CC, const Numeric CA, const Numeric CB, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

void	MPM93RainExt (MatrixView xsec, const Numeric CE, const Numeric CA, const Numeric CB, const String &model, ConstVectorView f_mono, ConstVectorView p_abs, ConstVectorView t_abs, ConstVectorView vmr)

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

Detailed Description

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

Author: Thomas Kuhn

Date: 2001-11-05

Definition in file continua.h.

Function Documentation

◆ BF86_CIA_N2()

void BF86_CIA_N2	(	MatrixView	xsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of N2-CIA according to BF-86 model [1/m]

Parameters

Cin	strength scaling factor [1]
model	allows user defined input parameter set (Cin) or choice of pre-defined parameters of specific models (see note below).
f_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	predefined temperature grid [K]
vmr	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 7762 of file continua.cc.

◆ check_continuum_model()

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 12724 of file continua.cc.

◆ CKD24_H20()

void CKD24_H20	(	MatrixView	xsec,
		int	isf,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr,
		ConstVectorView	n2_abs
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of H2O continuum according to CKD2.4 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	predefined temperature grid [K]
vmr	H2O volume mixing ratio profile [1]
n2_abs	N2 volume mixing ratio profile [1]

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: sbouk.nosp@m.aba@.nosp@m.aer.c.nosp@m.om, cloug.nosp@m.h@ae.nosp@m.r.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 5132 of file continua.cc.

◆ CKD_222_foreign_h2o()

void CKD_222_foreign_h2o	(	MatrixView	xsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr,
		ConstVectorView
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of H2O foreign continuum according to CKDv.2.2.2 [1/m]

Parameters

Cin	strength scaling factor [1]
model	allows user defined input parameter set (Cin) or choice of pre-defined parameters of specific models (see note below).
f_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	predefined temperature grid [K]
vmr	H2O volume mixing ratio profile [1]
n2_abs	N2 volume mixing ratio profile [1]

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 2381 of file continua.cc.

◆ CKD_222_self_h2o()

void CKD_222_self_h2o	(	MatrixView	xsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr,
		ConstVectorView
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of H2O self continuum according to CKD_2_2_2 [1/m]

Parameters

Cin	strength scaling factor [1]
model	allows user defined input parameter set (Cin) or choice of pre-defined parameters of specific models (see note below).
f_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	predefined temperature grid [K]
vmr	H2O volume mixing ratio profile [1]
n2_abs	N2 volume mixing ratio profile [1]

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 2093 of file continua.cc.

◆ CKD_241_co2()

void CKD_241_co2	(	MatrixView	xsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of CO2 continuum according to CKD_MT 1.00 [1/m]

Parameters

Cin	strength scaling factor [1]
model	allows user defined input parameter set (Cin) or choice of pre-defined parameters of specific models (see note below).
f_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	predefined temperature grid [K]
vmr	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 3611 of file continua.cc.

◆ CKD_242_foreign_h2o()

void CKD_242_foreign_h2o	(	MatrixView	xsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr,
		ConstVectorView
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of H2O foreign continuum according to CKDv.2.4.2 [1/m]

Parameters

Cin	strength scaling factor [1]
model	allows user defined input parameter set (Cin) or choice of pre-defined parameters of specific models (see note below).
f_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	predefined temperature grid [K]
vmr	H2O volume mixing ratio profile [1]
n2_abs	N2 volume mixing ratio profile [1]

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 2907 of file continua.cc.

◆ CKD_242_self_h2o()

void CKD_242_self_h2o	(	MatrixView	xsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr,
		ConstVectorView
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of H2O self continuum according to CKD_2_4_2 [1/m]

Parameters

Cin	strength scaling factor [1]
model	allows user defined input parameter set (Cin) or choice of pre-defined parameters of specific models (see note below).
f_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	predefined temperature grid [K]
vmr	H2O volume mixing ratio profile [1]
n2_abs	N2 volume mixing ratio profile [1]

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 2606 of file continua.cc.

◆ CKD_mt_100_foreign_h2o()

void CKD_mt_100_foreign_h2o	(	MatrixView	xsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr,
		ConstVectorView
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of H2O foreign continuum according to CKD_MT 1.00 [1/m]

Parameters

Cin	strength scaling factor [1]
model	allows user defined input parameter set (Cin) or choice of pre-defined parameters of specific models (see note below).
f_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	predefined temperature grid [K]
vmr	H2O volume mixing ratio profile [1]
n2_abs	N2 volume mixing ratio profile [1]

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.

◆ CKD_mt_100_self_h2o()

void CKD_mt_100_self_h2o	(	MatrixView	xsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr,
		ConstVectorView
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of H2O self continuum according to CKD_MT 1.00 [1/m]

Parameters

Cin	strength scaling factor [1]
model	allows user defined input parameter set (Cin) or choice of pre-defined parameters of specific models (see note below).
f_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	predefined temperature grid [K]
vmr	H2O volume mixing ratio profile [1]
n2_abs	N2 volume mixing ratio profile [1]

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 3152 of file continua.cc.

◆ CKD_mt_CIAfun_n2()

void CKD_mt_CIAfun_n2	(	MatrixView	xsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of N2-N2 CIA fundamental band according to CKD_MT 1.00 [1/m]

Parameters

Cin	strength scaling factor [1]
model	allows user defined input parameter set (Cin) or choice of pre-defined parameters of specific models (see note below).
f_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	predefined temperature grid [K]
vmr	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 4271 of file continua.cc.

◆ CKD_mt_CIAfun_o2()

void CKD_mt_CIAfun_o2	(	MatrixView	xsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of O2-O2 CIA fundamental band according to CKD_MT 1.00 [1/m]

Parameters

Cin	strength scaling factor [1]
model	allows user defined input parameter set (Cin) or choice of pre-defined parameters of specific models (see note below).
f_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	predefined temperature grid [K]
vmr	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 4484 of file continua.cc.

◆ CKD_mt_CIArot_n2()

void CKD_mt_CIArot_n2	(	MatrixView	xsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of N2-N2 CIA rot. band according to CKD_MT 1.00 [1/m]

Parameters

Cin	strength scaling factor [1]
model	allows user defined input parameter set (Cin) or choice of pre-defined parameters of specific models (see note below).
f_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	predefined temperature grid [K]
vmr	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 4020 of file continua.cc.

◆ CKD_mt_co2()

void CKD_mt_co2	(	MatrixView	xsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of CO2 continuum according to CKD_MT 1.00 [1/m]

Parameters

Cin	strength scaling factor [1]
model	allows user defined input parameter set (Cin) or choice of pre-defined parameters of specific models (see note below).
f_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	predefined temperature grid [K]
vmr	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 3808 of file continua.cc.

◆ CKD_mt_v0v0_o2()

void CKD_mt_v0v0_o2	(	MatrixView	xsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr,
		ConstVectorView	n2_abs
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of O2 v0<-v0 band according to CKD_MT 1.00 [1/m]

Parameters

Cin	strength scaling factor [1]
model	allows user defined input parameter set (Cin) or choice of pre-defined parameters of specific models (see note below).
f_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	predefined temperature grid [K]
vmr	O2 volume mixing ratio profile [1]
n2_abs	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 4705 of file continua.cc.

◆ CKD_mt_v1v0_o2()

void CKD_mt_v1v0_o2	(	MatrixView	xsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of O2 v1<-v0 band according to CKD_MT 1.00 [1/m]

Parameters

Cin	strength scaling factor [1]
model	allows user defined input parameter set (Cin) or choice of pre-defined parameters of specific models (see note below).
f_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	predefined temperature grid [K]
vmr	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 4910 of file continua.cc.

◆ CP98H2OAbsModel()

void CP98H2OAbsModel	(	MatrixView	xsec,
		const Numeric	CCin,
		const Numeric	CLin,
		const Numeric	CWin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of H2O (lines+continuum) according to Cruz-Pol 1998 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	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 1506 of file continua.cc.

◆ MaTipping_H2O_foreign_continuum()

void MaTipping_H2O_foreign_continuum	(	MatrixView	xsec,
		const Numeric	Cin,
		const Numeric	xin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of the H2O-dry air continuum [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure [Pa]
t_abs	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 1880 of file continua.cc.

◆ MPM85O2AbsModel()

void MPM85O2AbsModel	(	MatrixView	xsec,
		const Numeric	CCin,
		const Numeric	CLin,
		const Numeric	CWin,
		const Numeric	COin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	h2o_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of O2 according to MPM89 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure [Pa]
t_abs	predefined temperature grid [K]
h2o_abs	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 5563 of file continua.cc.

◆ MPM87H2OAbsModel()

void MPM87H2OAbsModel	(	MatrixView	xsec,
		const Numeric	CCin,
		const Numeric	CLin,
		const Numeric	CWin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of H2O (lines+continuum) according to MPM87 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	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 431 of file continua.cc.

◆ MPM87O2AbsModel()

void MPM87O2AbsModel	(	MatrixView	xsec,
		const Numeric	CCin,
		const Numeric	CLin,
		const Numeric	CWin,
		const Numeric	COin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	h2o_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of O2 according to MPM89 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure [Pa]
t_abs	predefined temperature grid [K]
h2o_abs	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 5846 of file continua.cc.

◆ MPM89H2OAbsModel()

void MPM89H2OAbsModel	(	MatrixView	xsec,
		const Numeric	CCin,
		const Numeric	CLin,
		const Numeric	CWin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of H2O (lines+continuum) according to MPM89 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	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 615 of file continua.cc.

◆ MPM89O2AbsModel()

void MPM89O2AbsModel	(	MatrixView	xsec,
		const Numeric	CCin,
		const Numeric	CLin,
		const Numeric	CWin,
		const Numeric	COin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	h2o_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of O2 according to MPM89 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure [Pa]
t_abs	predefined temperature grid [K]
h2o_abs	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 6121 of file continua.cc.

◆ MPM92O2AbsModel()

void MPM92O2AbsModel	(	MatrixView	xsec,
		const Numeric	CCin,
		const Numeric	CLin,
		const Numeric	CWin,
		const Numeric	COin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	h2o_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of O2 according to MPM93 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure [Pa]
t_abs	predefined temperature grid [K]
h2o_abs	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 6391 of file continua.cc.

◆ MPM93_H2O_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_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of H2O according to MPM87 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	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 5426 of file continua.cc.

◆ MPM93_N2_continuum()

void MPM93_N2_continuum	(	MatrixView	xsec,
		const Numeric	Cin,
		const Numeric	Gin,
		const Numeric	xTin,
		const Numeric	xfin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	h2o_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of N2-continuum according to MPM93 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	predefined temperature grid [K]
h2o_abs	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 7885 of file continua.cc.

◆ MPM93_O2_continuum()

void MPM93_O2_continuum	(	MatrixView	xsec,
		const Numeric	S0in,
		const Numeric	G0in,
		const Numeric	XS0in,
		const Numeric	XG0in,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	h2o_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of O2-continuum according to MPM93 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	predefined temperature grid [K]
h2o_abs	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 7323 of file continua.cc.

◆ MPM93H2OAbsModel()

void MPM93H2OAbsModel	(	MatrixView	xsec,
		const Numeric	CCin,
		const Numeric	CLin,
		const Numeric	CWin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of H2O (lines+continuum) according to MPM93 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	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 1075 of file continua.cc.

◆ MPM93IceCrystalAbs()

void MPM93IceCrystalAbs	(	MatrixView	xsec,
		const Numeric	CCin,
		const Numeric	CAin,
		const Numeric	CBin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of ice clouds according to MPM93 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	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 8714 of file continua.cc.

◆ MPM93O2AbsModel()

void MPM93O2AbsModel	(	MatrixView	xsec,
		const Numeric	CCin,
		const Numeric	CLin,
		const Numeric	CWin,
		const Numeric	COin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	h2o_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of O2 according to MPM93 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure [Pa]
t_abs	predefined temperature grid [K]
h2o_abs	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 6660 of file continua.cc.

◆ MPM93RainExt()

void MPM93RainExt	(	MatrixView	xsec,
		const Numeric	CEin,
		const Numeric	CAin,
		const Numeric	CBin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of water clouds according to MPM93 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	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 8876 of file continua.cc.

◆ MPM93WaterDropletAbs()

void MPM93WaterDropletAbs	(	MatrixView	xsec,
		const Numeric	CCin,
		const Numeric	CGin,
		const Numeric	CEin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of water clouds according to MPM93 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	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 8538 of file continua.cc.

◆ MPMLineShapeFunction()

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 9151 of file continua.cc.

◆ MPMLineShapeO2Function()

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 9208 of file continua.cc.

◆ Pardo_ATM_H2O_ForeignContinuum()

void Pardo_ATM_H2O_ForeignContinuum	(	MatrixView	xsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of N2-continuum according to Rosenkranz, 1993 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	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 5313 of file continua.cc.

◆ Pardo_ATM_N2_dry_continuum()

void Pardo_ATM_N2_dry_continuum	(	MatrixView	xsec,
		const Numeric	Cin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr,
		ConstVectorView	h2ovmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of N2-continuum according to Rosenkranz, 1993 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	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 8017 of file continua.cc.

◆ PWR93O2AbsModel()

void PWR93O2AbsModel	(	MatrixView	xsec,
		const Numeric	CCin,
		const Numeric	CLin,
		const Numeric	CWin,
		const Numeric	COin,
		const String &	model,
		const String &	version,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmrh2o,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of O2 according to the P. W. Rosenkranz, 1993 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure [Pa]
t_abs	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 6957 of file continua.cc.

◆ PWR98H2OAbsModel()

void PWR98H2OAbsModel	(	MatrixView	xsec,
		const Numeric	CCin,
		const Numeric	CLin,
		const Numeric	CWin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of H2O (lines+continuum) according to P. W. Rosenkranz, 1998 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	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 1299 of file continua.cc.

◆ Rosenkranz_CO2_foreign_continuum()

void Rosenkranz_CO2_foreign_continuum	(	MatrixView	xsec,
		const Numeric	Cin,
		const Numeric	xin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	n2_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of CO2-N2-continuum according to Rosenkranz, 1993 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	predefined temperature grid [K]
n2_abs	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 8433 of file continua.cc.

◆ Rosenkranz_CO2_self_continuum()

void Rosenkranz_CO2_self_continuum	(	MatrixView	xsec,
		const Numeric	Cin,
		const Numeric	xin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of CO2-CO2-continuum according to Rosenkranz, 1993 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	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 8334 of file continua.cc.

◆ Rosenkranz_N2_self_continuum()

void Rosenkranz_N2_self_continuum	(	MatrixView	xsec,
		const Numeric	Cin,
		const Numeric	xin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of N2-continuum according to Rosenkranz, 1993 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	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 8119 of file continua.cc.

◆ Rosenkranz_O2_continuum()

void Rosenkranz_O2_continuum	(	MatrixView	xsec,
		const Numeric	S0in,
		const Numeric	G0in,
		const Numeric	XS0in,
		const Numeric	XG0in,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	h2o_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of O2-continuum according to Rosenkranz 1993 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	predefined temperature grid [K]
h2o_abs	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 7468 of file continua.cc.

◆ Standard_H2O_foreign_continuum()

void Standard_H2O_foreign_continuum	(	MatrixView	xsec,
		const Numeric	Cin,
		const Numeric	xin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of the H2O-dry air continuum [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
t_abs	predefined temperature grid [K]
p_abs	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 1758 of file continua.cc.

◆ Standard_H2O_self_continuum()

void Standard_H2O_self_continuum	(	MatrixView	xsec,
		const Numeric	Cin,
		const Numeric	xin,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of the H2O-H2O continuum [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	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 1636 of file continua.cc.

◆ Standard_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_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	vmr
	)

Return values

xsec	cross section (absorption/volume mixing ratio) of N2-continuum according to Rosenkranz, 1993 [1/m]

Parameters

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_mono	predefined frequency grid [Hz]
p_abs	predefined pressure grid [Pa]
t_abs	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 8222 of file continua.cc.

◆ WVSatPressureIce()

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 9333 of file continua.cc.

◆ WVSatPressureLiquidWater()

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 9268 of file continua.cc.

◆ xsec_continuum_tag()

void xsec_continuum_tag	(	MatrixView	xsec,
		const String &	name,
		ConstVectorView	parameters,
		const String &	model,
		ConstVectorView	f_mono,
		ConstVectorView	p_abs,
		ConstVectorView	t_abs,
		ConstVectorView	n2_abs,
		ConstVectorView	h2o_abs,
		ConstVectorView	vmr
	)

Calculates model absorption for one continuum or full model tag.

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

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

Return values

xsec	Cross section of one continuum tag, xsec = alpha / VMR [1/m * 1]

Parameters

name	The name of the model to calculate (derived from the tag name)
parameters	model parameters, as defined in method cont_description_parameters.
model	model, related to model parameters
f_mono	Frequency grid [Hz]
p_abs	Pressure grid [Pa]
t_abs	Temperatures associated with the pressure grid, p_abs [K]
n2_abs	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]
h2o_abs	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 9392 of file continua.cc.

Variable Documentation

◆ addF77fields

const int addF77fields = 1

Definition at line 530 of file continua.h.

◆ FCO2_ckd_mt_100

const double FCO2_ckd_mt_100[FCO2_ckd_mt_100_npt+addF77fields]

Definition at line 3068 of file continua.h.

◆ FCO2_ckd_mt_100_dv

const Numeric FCO2_ckd_mt_100_dv = 10.0

Definition at line 3066 of file continua.h.

◆ FCO2_ckd_mt_100_npt

const int FCO2_ckd_mt_100_npt = 1003

Definition at line 3067 of file continua.h.

◆ FCO2_ckd_mt_100_v1

const Numeric FCO2_ckd_mt_100_v1 = -20.0

Definition at line 3064 of file continua.h.

◆ FCO2_ckd_mt_100_v2

const Numeric FCO2_ckd_mt_100_v2 = 10000.0

Definition at line 3065 of file continua.h.

◆ FH2O_ckd_0

const double FH2O_ckd_0[FH2O_ckd_0_npt+addF77fields]

Definition at line 971 of file continua.h.

◆ FH2O_ckd_0_dv

const Numeric FH2O_ckd_0_dv = 10.0

Definition at line 969 of file continua.h.

◆ FH2O_ckd_0_npt

const int FH2O_ckd_0_npt = 2003

Definition at line 970 of file continua.h.

◆ FH2O_ckd_0_v1

const Numeric FH2O_ckd_0_v1 = -20.0

Definition at line 967 of file continua.h.

◆ FH2O_ckd_0_v2

const Numeric FH2O_ckd_0_v2 = 20000.0

Definition at line 968 of file continua.h.

◆ FH2O_ckd_mt_100

const double FH2O_ckd_mt_100[FH2O_ckd_mt_100_npt+addF77fields]

Definition at line 2657 of file continua.h.

◆ FH2O_ckd_mt_100_dv

const Numeric FH2O_ckd_mt_100_dv = 10.0

Definition at line 2655 of file continua.h.

◆ FH2O_ckd_mt_100_npt

const int FH2O_ckd_mt_100_npt = 2003

Definition at line 2656 of file continua.h.

◆ FH2O_ckd_mt_100_v1

const Numeric FH2O_ckd_mt_100_v1 = -20.0

Definition at line 2653 of file continua.h.

◆ FH2O_ckd_mt_100_v2

const Numeric FH2O_ckd_mt_100_v2 = 20000.0

Definition at line 2654 of file continua.h.

◆ N2N2_CT220_ckd_mt_100

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 3313 of file continua.h.

◆ N2N2_CT220_ckd_mt_100_dv

const Numeric N2N2_CT220_ckd_mt_100_dv = 5.0

Definition at line 3311 of file continua.h.

◆ N2N2_CT220_ckd_mt_100_npt

const int N2N2_CT220_ckd_mt_100_npt = 73

Definition at line 3312 of file continua.h.

◆ N2N2_CT220_ckd_mt_100_v1

const Numeric N2N2_CT220_ckd_mt_100_v1 = -10.0

Definition at line 3309 of file continua.h.

◆ N2N2_CT220_ckd_mt_100_v2

const Numeric N2N2_CT220_ckd_mt_100_v2 = 350.0

Definition at line 3310 of file continua.h.

◆ N2N2_CT296_ckd_mt_100

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 3283 of file continua.h.

◆ N2N2_CT296_ckd_mt_100_dv

const Numeric N2N2_CT296_ckd_mt_100_dv = 5.0

Definition at line 3281 of file continua.h.

◆ N2N2_CT296_ckd_mt_100_npt

const int N2N2_CT296_ckd_mt_100_npt = 73

Definition at line 3282 of file continua.h.

◆ N2N2_CT296_ckd_mt_100_v1

const Numeric N2N2_CT296_ckd_mt_100_v1 = -10.0

Definition at line 3279 of file continua.h.

◆ N2N2_CT296_ckd_mt_100_v2

const Numeric N2N2_CT296_ckd_mt_100_v2 = 350.0

Definition at line 3280 of file continua.h.

◆ N2N2_N2F_ckd_mt_100

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 3341 of file continua.h.

◆ N2N2_N2F_ckd_mt_100_dv

const Numeric N2N2_N2F_ckd_mt_100_dv = 5.000

Definition at line 3339 of file continua.h.

◆ N2N2_N2F_ckd_mt_100_npt

const int N2N2_N2F_ckd_mt_100_npt = 118

Definition at line 3340 of file continua.h.

◆ N2N2_N2F_ckd_mt_100_v1

const Numeric N2N2_N2F_ckd_mt_100_v1 = 2085.000

Definition at line 3337 of file continua.h.

◆ N2N2_N2F_ckd_mt_100_v2

const Numeric N2N2_N2F_ckd_mt_100_v2 = 2670.000

Definition at line 3338 of file continua.h.

◆ N2N2_N2Ft_ckd_mt_100

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 3369 of file continua.h.

◆ O2_00_ckd_mt_100

const double O2_00_ckd_mt_100[O2_00_ckd_mt_100_npt+addF77fields]

Definition at line 3476 of file continua.h.

◆ O2_00_ckd_mt_100_dv

const Numeric O2_00_ckd_mt_100_dv = 2.000e0

Definition at line 3474 of file continua.h.

◆ O2_00_ckd_mt_100_npt

const int O2_00_ckd_mt_100_npt = 483

Definition at line 3475 of file continua.h.

◆ O2_00_ckd_mt_100_v1

const Numeric O2_00_ckd_mt_100_v1 = 7536.000e0

Definition at line 3472 of file continua.h.

◆ O2_00_ckd_mt_100_v2

const Numeric O2_00_ckd_mt_100_v2 = 8500.000e0

Definition at line 3473 of file continua.h.

◆ O2_10_ckd_mt_100_dv

const Numeric O2_10_ckd_mt_100_dv = 2.000e0

Definition at line 3593 of file continua.h.

◆ O2_10_ckd_mt_100_v1

const Numeric O2_10_ckd_mt_100_v1 = 9100.000e0

Definition at line 3591 of file continua.h.

◆ O2_10_ckd_mt_100_v2

const Numeric O2_10_ckd_mt_100_v2 = 11000.000e0

Definition at line 3592 of file continua.h.

◆ O2O2_O2F_ckd_mt_100_dv

const Numeric O2O2_O2F_ckd_mt_100_dv = 5.000

Definition at line 3405 of file continua.h.

◆ O2O2_O2F_ckd_mt_100_npt

const int O2O2_O2F_ckd_mt_100_npt = 103

Definition at line 3406 of file continua.h.

◆ O2O2_O2F_ckd_mt_100_v1

const Numeric O2O2_O2F_ckd_mt_100_v1 = 1340.000

Definition at line 3403 of file continua.h.

◆ O2O2_O2F_ckd_mt_100_v2

const Numeric O2O2_O2F_ckd_mt_100_v2 = 1850.000

Definition at line 3404 of file continua.h.

◆ O2O2_O2Fo_ckd_mt_100

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 3407 of file continua.h.

◆ O2O2_O2Ft_ckd_mt_100

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 3431 of file continua.h.

◆ SL260_ckd_0

const double SL260_ckd_0[SL260_ckd_0_npt+addF77fields]

Definition at line 1387 of file continua.h.

◆ SL260_ckd_0_dv

const Numeric SL260_ckd_0_dv = 10.0

Definition at line 1385 of file continua.h.

◆ SL260_ckd_0_npt

const int SL260_ckd_0_npt = 2003

Definition at line 1386 of file continua.h.

◆ SL260_ckd_0_v1

const Numeric SL260_ckd_0_v1 = -20.0

Definition at line 1383 of file continua.h.

◆ SL260_ckd_0_v2

const Numeric SL260_ckd_0_v2 = 20000.0

Definition at line 1384 of file continua.h.

◆ SL260_ckd_mt_100

const double SL260_ckd_mt_100[SL260_ckd_mt_100_npt+addF77fields]

Definition at line 2245 of file continua.h.

◆ SL260_ckd_mt_100_dv

const Numeric SL260_ckd_mt_100_dv = 10.0

Definition at line 2243 of file continua.h.

◆ SL260_ckd_mt_100_npt

const int SL260_ckd_mt_100_npt = 2003

Definition at line 2244 of file continua.h.

◆ SL260_ckd_mt_100_v1

const Numeric SL260_ckd_mt_100_v1 = -20.0

Definition at line 2241 of file continua.h.

◆ SL260_ckd_mt_100_v2

const Numeric SL260_ckd_mt_100_v2 = 20000.0

Definition at line 2242 of file continua.h.

◆ SL296_ckd_0

const double SL296_ckd_0[SL296_ckd_0_npt+addF77fields]

Definition at line 558 of file continua.h.

◆ SL296_ckd_0_dv

const Numeric SL296_ckd_0_dv = 10.0

Definition at line 556 of file continua.h.

◆ SL296_ckd_0_npt

const int SL296_ckd_0_npt = 2003

Definition at line 557 of file continua.h.

◆ SL296_ckd_0_v1

const Numeric SL296_ckd_0_v1 = -20.0

Definition at line 554 of file continua.h.

◆ SL296_ckd_0_v2

const Numeric SL296_ckd_0_v2 = 20000.0

Definition at line 555 of file continua.h.

◆ SL296_ckd_mt_100

const double SL296_ckd_mt_100[SL296_ckd_mt_100_npt+addF77fields]

Definition at line 1834 of file continua.h.

◆ SL296_ckd_mt_100_dv

const Numeric SL296_ckd_mt_100_dv = 10.0

Definition at line 1832 of file continua.h.

◆ SL296_ckd_mt_100_npt

const int SL296_ckd_mt_100_npt = 2003

Definition at line 1833 of file continua.h.

◆ SL296_ckd_mt_100_v1

const Numeric SL296_ckd_mt_100_v1 = -20.0

Definition at line 1830 of file continua.h.

◆ SL296_ckd_mt_100_v2

const Numeric SL296_ckd_mt_100_v2 = 20000.0

Definition at line 1831 of file continua.h.

Functions

Variables

Detailed Description

Function Documentation

◆ BF86_CIA_N2()

◆ check_continuum_model()

◆ 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()

◆ MaTipping_H2O_foreign_continuum()

◆ MPM85O2AbsModel()

◆ MPM87H2OAbsModel()

◆ MPM87O2AbsModel()

◆ MPM89H2OAbsModel()

◆ MPM89O2AbsModel()

◆ MPM92O2AbsModel()

◆ MPM93_H2O_continuum()

◆ MPM93_N2_continuum()

◆ MPM93_O2_continuum()

◆ MPM93H2OAbsModel()

◆ MPM93IceCrystalAbs()

◆ MPM93O2AbsModel()

◆ MPM93RainExt()

◆ MPM93WaterDropletAbs()

◆ MPMLineShapeFunction()

◆ MPMLineShapeO2Function()

◆ 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()

◆ WVSatPressureIce()

◆ WVSatPressureLiquidWater()

◆ xsec_continuum_tag()

Variable Documentation

◆ 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

◆ FH2O_ckd_0

◆ FH2O_ckd_0_dv

◆ FH2O_ckd_0_npt

◆ FH2O_ckd_0_v1

◆ FH2O_ckd_0_v2

◆ FH2O_ckd_mt_100

◆ FH2O_ckd_mt_100_dv

◆ FH2O_ckd_mt_100_npt

◆ FH2O_ckd_mt_100_v1

◆ FH2O_ckd_mt_100_v2

◆ 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

◆ N2N2_N2F_ckd_mt_100