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Probability Distribution for Coherent Transport of Random Waves

Yunrui Wang, Cheng Guo

Abstract

We establish a comprehensive probability theory for coherent transport of random waves through arbitrary linear media. The transmissivity distribution for random coherent waves is a fundamental B-spline with knots at the transmission eigenvalues. We analyze the distribution's shape, bounds, moments, and asymptotic behaviors. In the large n limit, the distribution converges to a Gaussian whose mean and variance depend solely on those of the eigenvalues. This result resolves the apparent paradox between bimodal eigenvalue distribution and unimodal transmissivity distribution.

Probability Distribution for Coherent Transport of Random Waves

Abstract

We establish a comprehensive probability theory for coherent transport of random waves through arbitrary linear media. The transmissivity distribution for random coherent waves is a fundamental B-spline with knots at the transmission eigenvalues. We analyze the distribution's shape, bounds, moments, and asymptotic behaviors. In the large n limit, the distribution converges to a Gaussian whose mean and variance depend solely on those of the eigenvalues. This result resolves the apparent paradox between bimodal eigenvalue distribution and unimodal transmissivity distribution.

Paper Structure

This paper contains 6 sections, 2 theorems, 31 equations, 6 figures.

Key Result

Theorem 1

The fundamental $B$-spline $M_{n-1}(t;\lambda_1, \ldots, \lambda_n)$ is the linear density function obtained by orthogonal projection onto the $t$-axis of an $(n-1)$-dimensional simplex $\sigma_{n-1}$ with unit volume, positioned such that its $n$ vertices project orthogonally onto the points $\lamb

Figures (6)

  • Figure 1: (a) Central problem: What is the probability distribution $p(t)$ of transmissivity $t$ for random coherent waves incident on a scattering medium? (b,c) Transmission eigenvalue distribution $p(\lambda_t)$ (red) versus Monte Carlo-simulated transmissivity distribution $p(t)$ (blue) for (b) fully chaotic and (c) diffusive systems. (d,e) Corresponding results for Bernoulli-distributed eigenvalues with (d) $q=0.5$ and (e) $q=0.8$.
  • Figure 2: (a) An $(n+m)$-port linear system transforms a coherent input wave $\bm{a}$ into a transmitted wave $\bm{b} = \tau \bm{a}$. (b-d) Transmissivity distribution $p_n(t)$ for $n=2, 3, 4$ input ports. Histograms show Monte Carlo results from $10^5$ random coherent inputs, blue curves show analytical B-spline predictions, and red dots and lines mark transmission eigenvalues $\bm{\lambda}(\tau^\dagger \tau)$.
  • Figure 3: Transmissivity distribution $p_n(t)$ for $n=5$ input ports. The blue curve shows the analytical result, with red dots and lines marking the transmission eigenvalues. The blue triangle indicates the mode $t_M$ (peak position), which is close to the Greville abscissa $\xi$ (red triangle). Orange- and purple-shaded regions indicate tail probabilities for extreme events.
  • Figure 4: Effects of eigenvalue degeneracy and asymptotic behavior. (a,b) Transmissivity distribution $p_4(t)$ with twofold and threefold eigenvalue degeneracy exhibits reduced smoothness at the degeneracy point. (c,d) Distributions $p_4(t)$ and $p_5(t)$ compared with their Gaussian approximations (orange dashed curves) demonstrate the central limit theorem.
  • Figure 5: Numerical demonstration of the theory. (a) A slab waveguide with permittivities $\varepsilon_i = 12.1$ (core), $\varepsilon = 2.1$ (cladding), and $\varepsilon_s = 2.0+0.86i$ (lossy scatterers), supporting $n=4$ TE modes. (b-d) Probability distributions for transmissivity $p_4(t)$, reflectivity $p_4(r)$, and absorptivity $p_4(\alpha)$. Histograms show Monte Carlo results from $10^5$ random coherent inputs, and solid curves show theoretical B-spline predictions.
  • ...and 1 more figures

Theorems & Definitions (4)

  • proof
  • Theorem : Curry and Schoenberg, 1966 curry1966
  • proof
  • Proposition : Curry and Schoenberg, 1966 curry1966