Radiative-transfer layer options
Select the within-layer approximation with
rte_option.
Option |
Within-layer model |
Step |
|---|---|---|
|
Endpoint-average propagation matrix and source |
Ordinary matrix exponential with a layer-average source. |
|
Constant propagation matrix and linear source |
Uses the linear-source operator \(\Lambda\) derived in Radiative Transfer. |
|
Linear propagation and linear source |
Uses the exact scalar linear-propagation source integral. Polarized transfer uses endpoint-average transmission with a commutator-free augmented-source correction. |
|
Linear propagation matrix and layer-average source |
Uses the second-order Magnus exponent and the ordinary source step. |
|
Linear propagation matrix and linear source |
Adds Magnus-ordered transmission to the augmented linear-source operator by retaining the first propagation-matrix commutator. |
All five options propagate analytical derivatives of their transmittance
and, where applicable, source operators. magop and magop_linsrc
are most useful when the polarized propagation matrices at the layer
endpoints do not commute. For scalar transfer, linprop evaluates the
linear-propagation source integral exactly. For polarized transfer,
linprop retains the ordinary endpoint-average transmission, whereas
magop_linsrc also includes the Magnus ordering correction.
See Radiative Transfer for the equations behind these options.