vSmartMOM principles

This page summarizes the core ideas behind vSmartMOM (vector Smart Matrix-Operator Method), consolidated from the primary references.

What problem vSmartMOM solves

  • Vector (polarized) radiative transfer in layered media with molecular (Rayleigh) and aerosol scattering, plus gaseous absorption.
  • Efficient, accurate multiple scattering using the matrix-operator method (doubling/adding) with discrete-ordinate quadrature.
  • Modular treatment of polarization states (I, IQ, IQU, IQUV) and Fourier decomposition in azimuth.
  • Optional linearization with respect to aerosol optical properties to facilitate Jacobians and sensitivity studies.

Method at a glance

  • Discretize angle with a quadrature (e.g., Gauss full-sphere, hemisphere, Radau) to get a finite set of streams.
  • Expand the vector phase matrix into Fourier series over azimuth and into Legendre polynomials over polar angle; use a truncation strategy.
  • Build per-layer single-scattering properties (optical thickness τ, single-scattering albedo ϖ, and polarized phase matrices Z⁺⁺, Z⁻⁺).
  • Compose layers via matrix-operator doubling/adding into a composite medium, preserving polarization.
  • Couple to surfaces via BRDF models (Lambertian, RPV, Ross–Li) in a vector-consistent way.

Truncation strategies and accuracy

  • δ-m and δ-fit approaches are used to remove/approximate strong forward peaks in scattering, improving convergence at low order.
  • vSmartMOM applies these truncations consistently to the vector phase matrix, following Sanghavi & Stephens (2015).
  • Practical guidance:
    • Choose L_trunc consistent with aerosol phase function complexity and desired accuracy.
    • Use Radau or Gauss full-sphere quadrature depending on hemispheric symmetry and source configuration.

Polarization handling

  • Supports Stokes vector subsets via fixed types: I; IQ; IQU; IQUV.
  • Phase matrix moments and the discrete-ordinate system are built per polarization type; this ensures type-stable kernels.

Linearization (aerosol Jacobians)

  • The matrix-operator formalism enables analytic derivatives with respect to aerosol properties (e.g., τ_ref, phase function parameters) by differentiating the composed operators.
  • vSmartMOM exposes aerosol optical property construction (Mie-based) and truncation, enabling efficient sensitivity calculations.

Layer optics and composition

  • Per-layer quantities include:
    • τλ (with gaseous absorption), ϖλ, τ, ϖ, and Fourier-expanded Z matrices.
    • Rayleigh properties are computed from depolarization factor and wavelength; aerosol properties from Mie models at reference λ.
  • Composition:
    • Added layer (A) and composite layer (C) operators are combined according to the standard matrix-operator algebra.
    • Doubling logic computes appropriate optical thickness sub-steps for numerical stability.

Surface interaction and HDRF

  • Surfaces are modeled via BRDFs; interaction terms are included in the boundary condition and in HDRF post-processing.
  • The HDRF and VZA postprocessing utilities provide azimuthal averaging and RAMI-style outputs.

Practical setup tips

  • Accuracy knobs: quadrature choice, L_trunc, max Fourier moment m, and depolarization factor for Rayleigh.
  • Stability: small per-step optical depths via doubling; ensure consistent units (wavenumber bands in cm⁻¹).
  • Performance: choose architecture CPU/GPU; GPU accelerates batched operations and kernel calls.

References

  • Sanghavi, S., Davis, A.B., Eldering, A. (2014). vSmartMOM: A vector matrix-operator method-based radiative transfer model linearized with respect to aerosol properties. JQSRT 133: 412–433.
  • Sanghavi, S., Stephens, G. (2015). Adaptation of the δ-m and δ-fit truncation methods to vector radiative transfer: Effect of truncation on radiative transfer accuracy. JQSRT 159: 53–68.
  • Grant, I.P., Hunt, G.E. (1969). Discrete space theory of radiative transfer I. Proc. Roy. Soc. A 313(1513): 183–197.
  • Plass, G.N., Kattawar, G.W., Catchings, F.E. (1973). Matrix operator theory of radiative transfer. 1: Rayleigh scattering. Applied Optics 12(2): 314–329.