RANDOM-MATRIX THEORY OF MESOSCOPIC FLUCTUATIONS IN CONDUCTORS AND SUPERCONDUCTORS

This paper contains a theoretical study of the sample-to-sample fluctuations in transport properties of phase-coherent, diffusive, quasi-one-dimensional systems. The main result is a formula for the variance of the fluctuations of an arbitrary linear statistic on the transmission eigenvalues [i.e., an observable of the form A = SIGMA(n=1)N f(T(n))]. The formula is the analog of the Dyson-Mehta theorem in the statistical theory of energy levels. The analysis is based on an existing random-matrix theory for the joint probability distribution of the transmission eigenvalues T(n) (n = 1, 2,..., N), and holds in the large-N limit. The variance of the fluctuations is shown to be independent of the sample size or degree of disorder and to have a universal 1/beta dependence on the symmetry parameter beta of the matrix ensemble. It follows that the universality which was established in the theory of ''universal conductance fluctuations'' is generic for a whole class of transport properties in mesoscopic conductors and superconductors. A further implication of the analysis is that the correlations between the transmission eigenvalues are not precisely described by a logarithmic interaction.