Lookup table (polarized) phase function (tabphase_polarized)#
Parameter |
Type |
Description |
Flags |
---|---|---|---|
m11 |
string |
A comma-separated list of phase matrix coefficient 1,1 of the phase function, parametrized by the cosine of the scattering angle. |
P |
m12 |
string |
A comma-separated list of phase matrix coefficient 1,2 of the phase function, parametrized by the cosine of the scattering angle. |
P |
m22 |
string |
A comma-separated list of phase matrix coefficient 2,2 of the phase function, parametrized by the cosine of the scattering angle. |
P |
m33 |
string |
A comma-separated list of phase matrix coefficient 3,3 of the phase function, parametrized by the cosine of the scattering angle. |
P |
m34 |
string |
A comma-separated list of phase matrix coefficient 3,4 of the phase function, parametrized by the cosine of the scattering angle. |
P |
m44 |
string |
A comma-separated list of phase matrix coefficient 4,4 of the phase function, parametrized by the cosine of the scattering angle. |
P |
nodes |
string |
A comma-separated list of \(\cos \theta\) specifying the grid on which values are defined. Bounds must be [-1, 1] and values must be strictly increasing. Must have the same length as values. |
P |
This plugin implements a generic phase function model for isotropic media parametrized by a lookup table giving values of the phase function as a function of the cosine of the scattering angle.
Notes
The scattering angle cosine is here defined as the dot product of the incoming and outgoing directions, where the incoming, resp. outgoing direction points toward, resp. outward the interaction point.
From this follows that \(\cos \theta = 1\) corresponds to forward scattering.
Lookup table points are regularly spaced between -1 and 1.
Phase function values are automatically normalized.
For polarized phase functions, this assumes (for the time being) the structure of a phase function with spherically symmetric particles, i.e. there are only four unique elements of the Mueller matrix: M_{11}, M_{12}, M_{33}, and M_{34}