Abstract

This article presents a method to simulate a three-dimensional (3D) electromagnetic Gaussian-Schell model (EGSM) source with desired characteristics. Using the complex screen method, originally developed for the synthesis of two-dimensional stochastic electromagnetic fields, a set of equations is derived which relate the desired 3D source characteristics to those of the statistics of the random complex screen. From these equations and the 3D EGSM source realizability conditions, a single criterion is derived, which when satisfied guarantees both the realizability and simulatability of the desired 3D EGSM source. Lastly, a 3D EGSM source, with specified properties, is simulated; the Monte Carlo simulation results are compared to the theoretical expressions to validate the method.

Highlights

  • The behavior of two-dimensional (2D) stochastic electromagnetic (EM) fields has and continues to be an important and popular topic of optics research [1,2,3,4,5,6]

  • Using the complex screen method [23,24,25], equations relating the desired 3D electromagnetic Gaussian-Schell model (EGSM) source parameters to the random complex screen parameters are derived. Using these equations and the realizability conditions developed in Ref. [22], a single criterion is found, which when satisfied guarantees that the desired 3D EGSM source is both realizable and simulatable

  • Any Γij combination that results in a point within the volume is both a realizable and simulatable 3D EGSM source

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Summary

Introduction

The behavior of two-dimensional (2D) stochastic electromagnetic (EM) fields has and continues to be an important and popular topic of optics research [1,2,3,4,5,6]. Using the complex screen method (originally developed for the synthesis of 2D random fields) [23,24,25], equations relating the desired 3D EGSM source parameters (source widths, spatial correlation radii, et cetera) to the random complex screen parameters are derived. Using these equations and the realizability conditions developed in Ref. This work can be put to immediate use in wave optics simulations of scenarios similar to those mentioned above

Theory
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