Crossover from bias-induced to field-induced breakdowns in one-dimensional band and Mott insulators attached to electrodes
arXiv:1101.2283 · doi:10.1103/PhysRevB.83.085113
Abstract
Nonequilibrium states induced by an applied bias voltage (V) and the corresponding current-voltage characteristics of one-dimensional models describing band and Mott insulators are investigated theoretically by using nonequilibrium Green's functions. We attach the models to metallic electrodes whose effects are incorporated into the self-energy. Modulation of the electron density and the scalar potential coming from the additional long-range interaction are calculated self-consistently within the Hartree approximation. For both models of band and Mott insulators with length L_C, the bias voltage induces a breakdown of the insulating state, whose threshold shows a crossover depending on L_C. It is determined basically by the bias for L_C smaller than the correlation length where W denotes the bandwidth and the energy gap. For systems with , the threshold is governed by the electric field, , which is consistent with a Landau-Zener-type breakdown, . We demonstrate that the spatial dependence of the scalar potential is crucially important for this crossover by showing the case without the scalar potential, where the breakdown occurs at regardless of the length L_C.
12 pages, 18 figures. To appear in Phys. Rev. B
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