Average optical path length estimation in a slab of arbitrary finite thickness

  • Tim Kindervatter
  • , Wei Li
  • , Nan Chen
  • , Yuping Huang
  • , Yongxiang Hu
  • , Snorre Stamnes
  • , Xiaomei Lu
  • , Børge Hamre
  • , Jakob J. Stamnes
  • , Tomonori Tanikawa
  • , Jennifer Lee
  • , Carl Weimer
  • , Xubin Zeng
  • , Charles K. Gatebe
  • , Knut Stamnes

Research output: Contribution to journalArticlepeer-review

Abstract

A method for determining the average photon path length in a slab of multiple scattering material is presented. Radiances can be obtained from the radiative transfer equation and subsequently differentiated to obtain the average photon path length. These radiances can be obtained via multiple methods including Monte Carlo simulations, analytic two-stream approximations, and multi-stream numerical solutions such as the AccuRT computational tool. Average path lengths obtained via numerical differentiation of these radiances are found to agree closely with path length estimates predicted by existing methods found in the literature. The average photon path length is further considered for a slab of finite physical thickness. It was found that for a slab consisting of non-absorbing material there is a linear relationship between the slab thickness and the average photon path length, but that for materials with nonzero absorption, this linear relationship breaks down as the slab thickness increases. Average path lengths may be converted to time spans to determine the amount of time a photon spends in a multiple scattering medium, which may be used to quantify the impact of multiple scattering on pulse stretching in lidar/radar applications.

Original languageEnglish
Article number1565245
JournalFrontiers in Remote Sensing
Volume6
DOIs
StatePublished - 2025

Keywords

  • lidar
  • multiple scattering
  • photon path length
  • radar
  • radiative transfer
  • two stream approximation

Fingerprint

Dive into the research topics of 'Average optical path length estimation in a slab of arbitrary finite thickness'. Together they form a unique fingerprint.

Cite this