Abstract

We study the probability distribution of the index N+{\mathcal N}_+, i.e., the number of positive eigenvalues of an N×NN\times N Gaussian random matrix. We show analytically that, for large NN and large N+\mathcal{N}_+ with the fraction 0≤c=N+/N≤10\le c=\mathcal{N}_+/N\le 1 of positive eigenvalues fixed, the index distribution P(N+=cN,N)∼exp⁡[−βN2Φ(c)]\mathcal{P}({\mathcal N}_+=cN,N)\sim\exp[-βN^2 Φ(c)] where ββ is the Dyson index characterizing the Gaussian ensemble. The associated large deviation rate function Φ(c)Φ(c) is computed explicitly for all 0≤c≤10\leq c \leq 1. It is independent of ββ and displays a quadratic form modulated by a logarithmic singularity around c=1/2c=1/2. As a consequence, the distribution of the index has a Gaussian form near the peak, but with a variance Δ(N)Δ(N) of index fluctuations growing as Δ(N)∼log⁡N/βπ2Δ(N)\sim \log N/βπ^2 for large NN. For β=2β=2, this result is independently confirmed against an exact finite NN formula, yielding Δ(N)=log⁡N/2π2+C+O(N−1)Δ(N)= \log N/2π^2 +C+\mathcal{O}(N^{-1}) for large NN, where the constant CC has the nontrivial value C=(γ+1+3log⁡2)/2π2≃0.185248...C=(γ+1+3\log 2)/2π^2\simeq 0.185248... and γ=0.5772...γ=0.5772... is the Euler constant. We also determine for large NN the probability that the interval [ζ1,ζ2][ζ_1,ζ_2] is free of eigenvalues. Part of these results have been announced in a recent letter [\textit{Phys. Rev. Lett.} {\bf 103}, 220603 (2009)].

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