# Pseudo-symmetric random matrices: semi-Poisson and sub-Wigner statistics

## TL;DR

This paper constructs ensembles of large pseudo-symmetric matrices with random elements, revealing their eigenvalue statistics follow sub-Wigner distributions related to physical phenomena like Anderson transitions and PT-symmetry.

## Contribution

It introduces a new class of pseudo-symmetric random matrices and characterizes their eigenvalue spacing distributions, connecting them to known physical transition phenomena.

## Key findings

- Eigenvalue spacings follow sub-Wigner distributions, especially semi-Poisson.
- Eigenvalue distributions fit well to a hyperbolic tangent-based function.
- The semi-Poisson distribution is closely related to 2x2 pseudo-symmetric matrix eigenvalues.

## Abstract

Real non-symmetric matrices may have either real or complex conjugate eigenvalues. These matrices can be seen to be pseudo-symmetric as $\eta M \eta^{-1} = M^t$, where the metric $\eta$ could be secular (a constant matrix) or depending upon the matrix elements of $M$. Here, we construct ensembles of a large number $N$ of pseudo-symmetric $n \times n$ ($n$ large) matrices using ${\cal N}$ $(n(n+1)/2 \le {\cal N} \le n^2)$ independent and identically distributed (iid) random numbers as their elements. Based on our numerical calculations, we conjecture that for these ensembles the Nearest Level Spacing Distributions (NLSDs: $p(s)$) are sub-Wigner as $p_{abc}(s)=a s e^{-bs^c} (0<c <2)$ and the distributions of their eigenvalues fit well to $D(\epsilon)= A[\mbox{tanh}\{(\epsilon+B)/C \}-\mbox{tanh}\{(\epsilon-B)/C\}]$ (exceptions also discussed). These sub-Wigner NLSD are encountered in Anderson metal-insulator transition and topological transitions in a Josephson junction. Interestingly, $p(s)$ for $c=1$ is called semi-Poisson and we show that it lies close to the form $p(s)=0.59 s K_0(0.45 s^2)$ derived for the case of $2 \times 2$ pseudo-symmetric matrix where the eigenvalues are most aptly conditionally real: $E_{1,2}=a \pm \sqrt{b^2-c^2}$ which represent characteristic coalescing of eigenvalues in PT(Parity-Time)-symmetric systems.