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Random Matrix Theory is a paradigm for describing and understanding a variety of phenomena in physics, mathematics, and potentially other disciplines. The theory was born in the early 1950s when theoretical physicist Eugene Wigner suggested that the problem of determining the energy level spacings of heavy nuclei – intractable by analytic means – might be modeled after the spectrum of a large random matrix. Originally conceived of as a statistical approach to systems with many degrees of freedom, Random Matrix Theory also applies to systems with few degrees of freedom whose classical dynamics is chaotic; in fact, Random Matrix Theory lies at the heart of one of the basic conjectures in Quantum Chaos. Formulated by Bohigas, Giannoni, and Schmit in 1984, this conjecture asserts that the eigenvalues of a quantized chaotic Hamiltonian (after suitable unfolding) behave like the spectrum of a typical member of the appropriate ensemble of random matrices. The Mathematics Department has a strong Random Matrix Theory Group consisting of Harold Widom (emeritus, UCSC), Alexander Gamburd and Torsten Ehrhardt. Harold Widom (emeritus, UCSC) and Craig Tracy (UC Davis) have made basic contributions to the theory. There are three basic classes of Random Matrix models, known as ‘GUE, GOE, and GSE’, for Glaussian Unitary, Orthogonal, and Symplectic ensembles, according to the type of matrix which is to be randomly selected. The limiting distribution (as the size of the matrix tends to infinity) for the largest eigenvaule in the GUE model had been computed via a Fredholm determinant by physicists. Widom and Tracy obtained the limiting distributions in the GOE and GSE models in terms of Fredholm determinants. They also showed that all three limiting distributions were representable in terms of Painleve functions, hence establishing connections to the theory of integrable dynamical systems. The resulting distributions are now universally knows as the Tracy-Widom distributions. It is believed to describe new universal limit laws for a wide variety of processes arising in mathematical physics and interacting particle systems. The distribution is destined to play an increasingly important role, akin to the bell curve, or normal distribution so familiar in statistics and probability. Alexander Gamburd Torsten Ehrhardt
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