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A Brownian-Motion Model for the Eigenvalues of a Random Matrix

Journal of Mathematical Physics · 1962 · Vol. 3(6) · pp. 1191–1198
Freeman J. Dyson

Abstract

A new type of Coulomb gas is defined, consisting of n point charges executing Brownian motions under the influence of their mutual electrostatic repulsions. It is proved that this gas gives an exact mathematical description of the behavior of the eigenvalues of an (n × n) Hermitian matrix, when the elements of the matrix execute independent Brownian motions without mutual interaction. By a suitable choice of initial conditions, the Brownian motion leads to an ensemble of random matrices which is a good statistical model for the Hamiltonian of a complex system possessing approximate conservation laws. The development with time of the Coulomb gas represents the statistical behavior of the eigenvalues of a complex system as the strength of conservation-destroying interactions is gradually increased. A ``virial theorem'' is proved for the Brownian-motion gas, and various properties of the stationary Coulomb gas are deduced as corollaries.

Random Matrices and ApplicationsStochastic processes and statistical mechanicsTheoretical and Computational PhysicsEigenvalues and eigenvectorsRandom matrixBrownian motionCoulombHermitian matrixHamiltonian (control theory)Classical mechanicsMathematicsPhysicsStatistical physics
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References
On the Theory of the Brownian Motion
Physical Review · 1930 · 4,464 citations
Statistical Theory of the Energy Levels of Complex Systems. I
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