Introduction to Random Matrices
Abstract
These notes provide an introduction to the theory of random matrices. The central quantity studied is τ(a)= det(1-K) where K is the integral operator with kernel 1/π π(x-y) x-y I(y). Here I=j(a2j-1,a2j) and I(y) is the characteristic function of the set I. In the Gaussian Unitary Ensemble (GUE) the probability that no eigenvalues lie in I is equal to τ(a). Also τ(a) is a tau-function and we present a new simplified derivation of the system of nonlinear completely integrable equations (the aj's are the independent variables) that were first derived by Jimbo, Miwa, M\ori, and Sato in 1980. In the case of a single interval these equations are reducible to a Painlev\'e V equation. For large s we give an asymptotic formula for E2(n;s), which is the probability in the GUE that exactly n eigenvalues lie in an interval of length s.
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