Fig. 1

Top: definition of the incident, s′, and
emergent, s, photon directions at a
scattering event within the atmosphere. The xyz axes form a rest
reference frame fixed to the planet. The differential solid angle dΩ(s′) =
sinθdθdφ is defined with
s serving as polar axis. Angles
θ ∈ [
0,π] and φ ∈[0,
2π].
In the backtracing of photons of BMC algorithms, s is
known at each collision and s′
must be sampled from the relevant scattering phase function. Angles i′ and
i,
both ∈[0,
π],
are needed for consistent referencing of the Stokes vector throughout the scattering
process. Vectors {,
and
} and {e1,
e2 and
e3}
define right-handed coordinate systems at the meridional planes of the incident and
emergent photon directions, respectively. Bottom: definition of the
incident, s′,
and emergent, s, photon directions at a
reflection event at the local surface (plane
).
Here, n is the inward-pointing normal
vector at the surface, and ẑ is oriented along −n. The
differential solid angle dΩ(s′) =
sinθdθdφ is defined with
ẑ
serving as polar axis.
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