Abstract:
We investigate disorder-induced localization in metals that break time-reversal and inversion symmetries through their energy dispersion, ϵk≠ϵ-k, but lack Berry phases. In the perturbative regime of disorder, we show that weak localization is suppressed due to a mismatch of the Fermi velocities of left and right movers. To substantiate this analytical result, we perform quench numerics on chains shorter than the Anderson localization length ζ - the latter computed and verified to be finite using the recursive Green's function method - and find a sharp rise in the saturation value of the participation ratio due to band asymmetry, indicating a tendency to delocalize. Interestingly, for weak disorder strength η, we see a better fit to the scaling behavior ζ∝1/η2 for asymmetric bands than conventional symmetric ones.
