Abstract

Experimental and theoretical investigations of the distribution of Coulomb blockade peak spacings in chaotic quantum dots have shown a significant deviation from the Wigner–Dyson distribution predicted by the constant interaction model. Recently we introduced a random interaction matrix model for chaotic or diffusive dots that describes the crossover of the peak spacing statistics from a Wigner–Dyson distribution to a Gaussian-like distribution. Here we use this model to study the dependence of the peak-spacing distributions on the underlying space-time symmetries of the one-body Hamiltonian, and in particular we compare the cases of conserved and broken time-reversal symmetry. We also study the dependence of the peak spacing fluctuations on disorder strength in diffusive dots using a standard tight-binding Hamiltonian with Coulomb interactions. The fluctuations are found to increase with disorder and can be related to the disorder-enhanced fluctuations of the interaction matrix elements.

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