Giant Nernst Effect due to Fluctuating Cooper Pairs in Superconductors
M. N. Serbyn, M. A. Skvortsov, A. A. Varlamov, Victor Galitski

TL;DR
This paper develops a comprehensive theory for the giant Nernst effect caused by fluctuating Cooper pairs in two-dimensional superconductors, explaining experimental observations across various conditions.
Contribution
It introduces a simple phenomenological formula and a microscopic calculation for the fluctuation-induced Nernst effect, extending understanding beyond the upper critical field.
Findings
The Nernst signal can be significantly large even far from the transition.
The theoretical results match experimental data in disordered superconducting films.
The study provides asymptotic dependencies of the Nernst coefficient in different phase diagram regions.
Abstract
A theory of the fluctuation-induced Nernst effect is developed for arbitrary magnetic fields and temperatures beyond the upper critical field line in a two-dimensional superconductor. First, we derive a simple phenomenological formula for the Nernst coefficient, which naturally explains the giant Nernst signal due to fluctuating Cooper pairs. The latter is shown to be large even far from the transition and may exceed by orders of magnitude the Fermi liquid terms. We also present a complete microscopic calculation (which includes quantum fluctuations) of the Nernst coefficient and give its asymptotic dependencies in various regions on the phase diagram. It is argued that the magnitude and the behavior of the Nernst signal observed experimentally in disordered superconducting films can be well-understood on the basis of the superconducting fluctuation theory.
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