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Introduction to Random Matrices

High Energy Physics - Theory 2015-06-26 v1 Condensed Matter Mathematical Physics math.MP Exactly Solvable and Integrable Systems solv-int

Abstract

These notes provide an introduction to the theory of random matrices. The central quantity studied is τ(a)=det(1K)\tau(a)= det(1-K) where KK is the integral operator with kernel 1/\pi} {\sin\pi(x-y)\over x-y} \chi_I(y). Here I=j(a2j1,a2j)I=\bigcup_j(a_{2j-1},a_{2j}) and χI(y)\chi_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)\tau(a). Also τ(a)\tau(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{\^o}ri, and Sato in 1980. In the case of a single interval these equations are reducible to a Painlev{\'e} 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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Cite

@article{arxiv.hep-th/9210073,
  title  = {Introduction to Random Matrices},
  author = {Craig A. Tracy and Harold Widom},
  journal= {arXiv preprint arXiv:hep-th/9210073},
  year   = {2015}
}

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44 pages