Pu and Korotkova (Optics Communications 283, 1693, 2010) derived propagation laws for the spectral density and polarization of stochastic electromagnetic beams — modeled as electromagnetic Gaussian Schell-model (EMGSM) sources — traveling through linear, deterministic media whose complex wave numbers , for the two polarization components are constant along the propagation direction, using paraxial ABCD (ray-matrix) propagation. Their analysis rests on explicit simplifying assumptions that delineate five extension directions: (1) longitudinally varying, stratified, or otherwise inhomogeneous media; (2) statistically random (turbulent) media; (3) nonparaxial or full-vector Maxwell propagation; (4) nonlinear medium response such as gain saturation or an intensity-dependent refractive index; and (5) experimental validation and source classes beyond EMGSM. Directions (1), (2), (5), and the free-space part of (3) have direct treatments in the same cross-spectral-density-matrix framework [4–8, 10, 11, 16–18, 21]; no direct treatment is known for stochastic electromagnetic beams (fluctuating polarization, 2x2 cross-spectral-density matrix) in media with nonlinear response, or for a full-vector nonparaxial treatment in linear gain or absorbing media. The problem is therefore the surviving core: derive and validate propagation laws for the cross-spectral-density matrix of stochastic electromagnetic beams in media with nonlinear response — gain-saturated active media or Kerr-type media with an intensity-dependent refractive index — and under full-vector nonparaxial propagation in linear gain or absorbing media, such that the published linear paraxial laws are recovered in the limits specified in the Problem Statement; the nonlinear and nonparaxial regimes, and the two nonlinearity classes, are independent targets, each sufficient on its own.
Background
A stochastic (random) electromagnetic beam is a beam whose electric field components fluctuate statistically in space and time; its second-order properties are described, at a single frequency , by the 2x2 cross-spectral density (CSD) matrix with entries , where the indices and label two mutually orthogonal transverse polarization components. The spectral density (the spectrum at a point) is ; the spectral degree of coherence between two points is the normalized trace of the CSD matrix; and the degree of polarization at a point is , ranging from 0 (unpolarized) to 1 (fully polarized). Wolf's unified theory of coherence and polarization (2003) established that coherence and polarization are two aspects of this one matrix, and that all three quantities generally change on propagation, even in free space, through correlation-induced effects.
A workhorse source model is the electromagnetic Gaussian Schell-model (EMGSM) beam, for which the spectral density of each component is Gaussian and the degrees of coherence between all component pairs are Gaussian functions of the separation of the two points. Its propagation through deterministic first-order (ABCD) optical systems — systems, such as free space, thin lenses, and quadratic media, in which the transverse ray coordinates transform linearly under paraxial (small-angle) propagation — can be computed by the generalized Huygens–Fresnel integral.
Pu and Korotkova (2010) combined these tools for a medium with gain or absorption, modeled by complex wave numbers , whose real parts are refractive indices and whose imaginary parts describe gain or absorption; the two polarization components may be amplified or attenuated differently (dichroism). They derived how the spectral density, the degree of coherence, and the degree of polarization of EMGSM beams evolve in such media, showing for example that the degree of polarization can be controlled by the dispersion of the complex wave numbers. The analysis rests on explicit simplifying assumptions: the medium is linear, deterministic, and uniform along the propagation direction (, independent of ), and propagation is paraxial within the ABCD formalism, with free-space propagation used in the numerical examples. These assumptions are the scope limits of the 2010 theory; the problem asks for the theory to be extended beyond them.
Substantial adjacent work exists. Turbulent (statistically random) media were treated within the same CSD framework by Salem, Korotkova, Dogariu, and Wolf (2004) for atmospheric turbulence, by Korotkova, Salem, and Wolf (2004), Korotkova, Salem, Dogariu, and Wolf (2005), and Korotkova and Gbur (2007), and by Pu and Korotkova themselves (2009) for the degree of cross-polarization in a turbulent atmosphere. Korotkova and Farwell (2010, 2011) extended this to oceanic turbulence, whose power spectrum mixes temperature and salinity fluctuations; Yao, Toselli, and Korotkova (2014) and Korotkova (2015) treated anisotropic turbulence. Related spectral analyses for deterministic media with general refractive properties, including negative-phase (negative-index) materials, were given by Tong and Korotkova (2010). Lahiri and Wolf (2013) developed the propagation theory for beams of any state of coherence and polarization through multilayered stratified media. Nonparaxial stochastic electromagnetic beams in free space were analyzed by Zhu and Zhao (2009) and Ding and coauthors (2011). Source classes beyond EMGSM include electromagnetic multi-Gaussian, cosine-Gaussian, vortex, and rectangular multi-Gaussian Schell-model beams (Mei, Korotkova, and Shchepakina 2012; Mei and Korotkova 2013; Chen and Pu 2008; Chen and Zhao 2016), and Avramov-Zamurovic and coauthors (2016) reported laboratory measurements of electromagnetic Bessel-Gaussian Schell-model beams in a turbulent channel. For the nonlinear regime, the adjacent literature treats mutually incoherent vector soliton pairs in saturable or self-focusing media (Litchinitser and coauthors, 1999; Yang and Pelinovsky, 2003; Ponomarenko and Agrawal, 2004; Motzek and coauthors, 2004) and deterministic filamentation instability of electromagnetic beams (Sodha and Faisal, 2017), but does not deliver propagation laws for the CSD matrix, spectral density, or polarization in the unified coherence–polarization framework; follow-up work on partially coherent beams in gain or absorbing media (Yang and coauthors, 2021) keeps the medium response linear.
Problem Statement
Pu and Korotkova (2010) obtained the evolution laws for the 2x2 cross-spectral-density (CSD) matrix and the derived spectral density, spectral degree of coherence, and degree of polarization for linear, deterministic, z-uniform gain/absorbing media under paraxial ABCD propagation. Extending this propagation theory to more general propagation environments is the problem posed here: (i) media whose complex wave numbers vary along the propagation direction or are spatially non-uniform, such as stratified or inhomogeneous media; (ii) statistically random (turbulent) media; (iii) nonparaxial propagation or situations requiring a full-vector Maxwell treatment; (iv) media with nonlinear response, such as gain saturation or an intensity-dependent refractive index; and (v) experimental validation and source classes beyond the EMGSM family. Because (i), (ii), (v), and the free-space portion of (iii) already have direct treatments in the literature [4–8, 10, 11, 16–18, 21], the surviving open core is the following. For a stochastic electromagnetic beam with a general admissible 2x2 CSD matrix (fluctuating polarization; the EMGSM family is the case underlying the published laws), derive and validate propagation laws for the CSD matrix in media with nonlinear response — either a gain-saturated active medium or a Kerr-type medium with an intensity-dependent refractive index, each independently sufficient — and, independently, for full-vector nonparaxial propagation in linear gain or absorbing media with complex wave numbers , . Each of these two regimes is a separately sufficient target, and within the nonlinear regime either nonlinearity class likewise suffices on its own; no target is conditional on another. For the regime treated, the law must give the full CSD matrix and the derived spectral density , spectral degree of coherence , and degree of polarization , and must reduce to the known linear, deterministic, z-uniform, paraxial results of Pu and Korotkova in the limit of vanishing nonlinear response (zero intensity-dependent index; linear gain/absorption) for the nonlinear regime, and in the paraxial (small-angle) limit for the nonparaxial regime.
References
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