arXiv2001
We model the effect of phase-breaking collisions on the coherent electron transport in a disordered one-dimensional single-channel wire. In our model the phase-breaking collisions break the wire into segments, where each segment is an independent series resistor with coherent electronic resistance and the segmentation is a stochastic process with Poisson distribution of phase-breaking scattering times. The wire resistance as a function of the wire length $L$, coherence length $L_ϕ$, and localisation length $ξ$ is calculated and the transition from coherent to incoherent transport is traced quantitatively. In the coherent regime ($L < L_ϕ$) the resistance fluctuates from wire to wire with a characteristic log-normal distribution of resistances, the typical resistance increases as $\exp(L/ξ)$, and the mean resistance increases as $\exp(2L/ξ)$ (or faster if disorder is strong). As $L$ exceeds $L_ϕ$, decoherence suppresses the resistance fluctuations and narrows the resistance distribution. As a result, at $L \gg L_ϕ$ the mean resistance increases as $βL-c$ and the typical resistance as $βL - c'$, where $β$ is the wire resistivity, $c$ is a constant shift due to the decoherence near the source electrode, and $c' \gg c$ is the shift related to the resistance self-averaging in a single wire. Numerical results are given for a GaAs quantum wire. It is noted that coherent transport in such wire can exhibit peculiar deviations from universal scaling owing to strong backscattering by impurities.