Weak localization of disordered quasiparticles in the mixed superconducting state
R. Bundschuh, C. Cassanello, D. Serban, M.R. Zirnbauer

TL;DR
This paper develops a nonlinear sigma model to describe weak localization effects on quasiparticles in disordered superconductors in the mixed state, explaining experimental thermal conductivity behavior.
Contribution
It introduces a symmetry-based supermatrix field theory for quasiparticles in disordered superconductors and links weak localization to thermal conductivity variations.
Findings
Weak localization correction affects thermal conductivity near H_c1
Zeeman splitting cuts off localization effects at low temperatures
Model explains field dependence observed in high-T_c experiments
Abstract
Starting from a random matrix model, we construct the low-energy effective field theory for the noninteracting gas of quasiparticles of a disordered superconductor in the mixed state. The theory is a nonlinear sigma model, with the order parameter field being a supermatrix whose form is determined solely on symmetry grounds. The weak localization correction to the field-axis thermal conductivity is computed for a dilute array of s-wave vortices near the lower critical field H_c1. We propose that weak localization effects, cut off at low temperatures by the Zeeman splitting, are responsible for the field dependence of the thermal conductivity seen in recent high-T_c experiments by Aubin et al.
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