paper

Quantum and Boltzmann transport in the quasi-one-dimensional wire with rough edges

arXiv:1011.6193 · doi:10.1103/PhysRevB.83.245328

Abstract

We study quantum transport in Q1D wires made of a 2D conductor of width W and length L>>W. Our aim is to compare an impurity-free wire with rough edges with a smooth wire with impurity disorder. We calculate the electron transmission through the wires by the scattering-matrix method, and we find the Landauer conductance for a large ensemble of disordered wires. We study the impurity-free wire whose edges have a roughness correlation length comparable with the Fermi wave length. The mean resistance <ρ> and inverse mean conductance 1/<g> are evaluated in dependence on L. For L -> 0 we observe the quasi-ballistic dependence 1/<g> = <ρ> = 1/N_c + ρ_{qb} L/W, where 1/N_c is the fundamental contact resistance and ρ_{qb} is the quasi-ballistic resistivity. As L increases, we observe crossover to the diffusive dependence 1/<g> = <ρ> = 1/N^{eff}_c + ρ_{dif} L/W, where ρ_{dif} is the resistivity and 1/N^{eff}_c is the effective contact resistance corresponding to the N^{eff}_c open channels. We find the universal results ρ_{qb}/ρ_{dif} = 0.6N_c and N^{eff}_c = 6 for N_c >> 1. As L exceeds the localization length ξ, the resistance shows onset of localization while the conductance shows the diffusive dependence 1/<g> = 1/N^{eff}_c + ρ_{dif} L/W up to L = 2ξand the localization for L > 2ξonly. On the contrary, for the impurity disorder we find a standard diffusive behavior, namely 1/<g> = <ρ> = 1/N_c + ρ_{dif} L/W for L < ξ. We also derive the wire conductivity from the semiclassical Boltzmann equation, and we compare the semiclassical electron mean-free path with the mean free path obtained from the quantum resistivity ρ_{dif}. They coincide for the impurity disorder, however, for the edge roughness they strongly differ, i.e., the diffusive transport is not semiclassical. It becomes semiclassical for the edge roughness with large correlation length.

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