Abstract
In this article, the motion of a single quantum particle on a lattice with stochastically fluctuating site energies is investigated. The model is characterized by three parameters: the matrix elementJ for coherent energy transfer between nearest neighbours and the strength Δ and correlation time 1/γ of the fluctuations. Because of the simple structure of its Hamiltonian, expressions for stochastic moments such as the mean square displacement can be derived, which are valid for strong fluctuations, no matter how slow their decay, and for weak fluctuations, in the short correlation time limit. The basic idea of the method is to treat the deterministic part of the motion as perturbation acting on the stochastic part. While this method was previously used to obtain the diffusion constant for fluctuations represented by dichotomic Markov processes (DMPs), now the more realistic situation of Gaussian Markov processes is treated. The resulting diffusion constants are compared with those of dichotomic systems. Major differences appear for strong fluctuations and long correlation times. Contrary to the DMP case, the diffusion constant turns out to be a monotonously increasing function of the inverse correlation time γ (withJ, Δ fixed), for all values of γ. Anderson localization is observed at γ=0 but disappears as γ increases.
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Kassner, K. Quantum diffusion on a lattice with gaussian fluctuating site energies. Z. Physik B - Condensed Matter 70, 229–239 (1988). https://doi.org/10.1007/BF01318305
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DOI: https://doi.org/10.1007/BF01318305