Abstract

These notes provide an introduction to the theory of random matrices. The central quantity studied is τ(a)=det(1−K)τ(a)= det(1-K) where KK is the integral operator with kernel $1/π} {\sinπ(x-y)\over x-y} χ_I(y)$. Here I=⋃j(a2j−1,a2j)I=\bigcup_j(a_{2j-1},a_{2j}) and χI(y)χ_I(y) is the characteristic function of the set II. In the Gaussian Unitary Ensemble (GUE) the probability that no eigenvalues lie in II is equal to τ(a)τ(a). Also τ(a)τ(a) is a tau-function and we present a new simplified derivation of the system of nonlinear completely integrable equations (the aja_j's are the independent variables) that were first derived by Jimbo, Miwa, M{ô}ri, and Sato in 1980. In the case of a single interval these equations are reducible to a Painlev{é} V equation. For large ss we give an asymptotic formula for E2(n;s)E_2(n;s), which is the probability in the GUE that exactly nn eigenvalues lie in an interval of length ss.

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