spectral_rad_srcvec_pathFromPropmat
- Workspace.spectral_rad_srcvec_pathFromPropmat(self, spectral_rad_srcvec_path: pyarts3.arts.SourceVector | None = None, spectral_propmat_path: pyarts3.arts.ArrayOfPropmatVector | None = None, spectral_nlte_srcvec_path: pyarts3.arts.ArrayOfStokvecVector | None = None, spectral_propmat_jac_path: pyarts3.arts.ArrayOfPropmatMatrix | None = None, spectral_nlte_srcvec_jac_path: pyarts3.arts.ArrayOfStokvecMatrix | None = None, freq_grid_path: pyarts3.arts.ArrayOfAscendingGrid | None = None, atm_path: pyarts3.arts.ArrayOfAtmPoint | None = None, jac_targets: pyarts3.arts.JacobianTargets | None = None) None
Gets the source term along the path.
Per
Stokvecelement (single frequency, single temperature, single derivative target), the source term is computed as:\[\vec{J} = B(T, f) + \mathbf{K}^{-1} \vec{S}\]and the Jacobian is computed as:
\[\frac{\partial \vec{J}}{\partial x} = \frac{\partial B(T, f)}{\partial x} - \mathbf{K}^{-1} \left( \frac{\partial \mathbf{K}}{\partial x} \mathbf{K}^{-1} - \frac{\partial \vec{S}}{\partial x} \right)\]where:
Variable
Extracted from ARTS parameter
Meaning
\(\vec{J}\)
spectral_rad_srcvec_pathJThe spectral radiance source term along the path.
\(B(T, f)\)
None- this is computed locallyThe Planck function at the temperature and frequency.
\(\mathbf{K}\)
spectral_propmat_pathThe propagation matrix along the path.
\(\vec{S}\)
spectral_nlte_srcvec_pathThe non-LTE source vector along the path.
\(\frac{\partial \vec{J}}{\partial x}\)
spectral_rad_srcvec_pathdJThe Jacobian of the spectral radiance source term with respect to the
jac_targets.\(\frac{\partial B(T, f)}{\partial x}\)
None- this is computed locallyThe Jacobian of the Planck function with respect to the
jac_targets. Only tempertature is supported.\(\frac{\partial \mathbf{K}}{\partial x}\)
spectral_propmat_jac_pathThe Jacobian of the propagation matrix with respect to the
jac_targets.\(\frac{\partial \vec{S}}{\partial x}\)
spectral_nlte_srcvec_jac_pathThe Jacobian of the non-LTE source vector with respect to the
jac_targets.\(x\)
jac_targetsThe targets for the Jacobian computation.
\(T\)
atm_pathThe temperature at the atmospheric point along the path.
\(f\)
freq_grid_pathThe frequency grid at the atmospheric point along the path.
The output dimensions are:
spectral_rad_srcvec_path:freq_gridxray_path,freq_gridxray_pathxjac_targets(target count)
Author: Richard Larsson
Used by wrapper methods
spectral_radClearskyEmission()spectral_radClearskyRayleighScattering()spectral_radClearskyScattering()
- Parameters:
spectral_rad_srcvec_path (SourceVector, optional) – Source vectors along the propagation path. See
spectral_rad_srcvec_path, defaults toself.spectral_rad_srcvec_path[OUT]spectral_propmat_path (ArrayOfPropmatVector, optional) – Propagation matrices along the propagation path. See
spectral_propmat_path, defaults toself.spectral_propmat_path[IN]spectral_nlte_srcvec_path (ArrayOfStokvecVector, optional) – Additional non-LTE along the propagation path. See
spectral_nlte_srcvec_path, defaults toself.spectral_nlte_srcvec_path[IN]spectral_propmat_jac_path (ArrayOfPropmatMatrix, optional) – Propagation derivative matrices along the propagation path. See
spectral_propmat_jac_path, defaults toself.spectral_propmat_jac_path[IN]spectral_nlte_srcvec_jac_path (ArrayOfStokvecMatrix, optional) – Additional non-LTE derivative along the propagation path. See
spectral_nlte_srcvec_jac_path, defaults toself.spectral_nlte_srcvec_jac_path[IN]freq_grid_path (ArrayOfAscendingGrid, optional) – All
freq_gridalong the propagation path. Seefreq_grid_path, defaults toself.freq_grid_path[IN]atm_path (ArrayOfAtmPoint, optional) – Atmospheric points along the propagation path. See
atm_path, defaults toself.atm_path[IN]jac_targets (JacobianTargets, optional) – A list of targets for the Jacobian Matrix calculations. See
jac_targets, defaults toself.jac_targets[IN]