Abstract
We consider a charged quantum particle in a two-dimensional disordered system subject to a spatially and temporally fluctuating magnetic field. The fluctuations are assumed to be Gaussian, with correlations typical for a metal in the anomalous-skin-effect regime. We derive a scaling form for the quantum correction to the conductivity in terms of a scaled temperature, elastic mean free path, and magnetic field. The weak localization correction to the conductivity is calculated for the case of rapid magnetic-field fluctuations. We express the result in terms of a phenomenological phase relaxation rate 1/τφ*, which is found to scale with temperature as T1/3, provided the potential disorder is sufficiently strong and the temperature is above a critical value. In all other cases, including the normal-skin-effect regime and the case of quasistatic field fluctuations, 1/τφ is found to be proportional to T, albeit with unusual prefactors.