Larkin-Ovchinnikov-Fulde-Ferrell state in quasi-one-dimensional superconductors
N. Dupuis

TL;DR
This paper explores the phase diagram of quasi-one-dimensional superconductors under magnetic fields, highlighting conditions for the LOFF state and its experimental signatures, especially in Bechgaard salts and related organic materials.
Contribution
It provides a detailed theoretical analysis of the LOFF state in quasi-1D superconductors, including phase diagrams and experimental implications, emphasizing the role of anisotropy.
Findings
High-field superconducting phases are stabilized by dimensional crossover.
Experimental data on (TMTSF)$_2$ClO$_4$ align with theoretical predictions.
Large anisotropy enhances the likelihood of observing the LOFF state.
Abstract
The properties of a quasi-one-dimensional (quasi-1D) superconductor with {\it an open Fermi surface} are expected to be unusual in a magnetic field. On the one hand, the quasi-1D structure of the Fermi surface strongly favors the formation of a non-uniform state (Larkin-Ovchinnikov-Fulde-Ferrell (LOFF) state) in the presence of a magnetic field acting on the electron spins. On the other hand, a magnetic field acting on an open Fermi surface induces a dimensional crossover by confining the electronic wave-functions wave-functions along the chains of highest conductivity, which results in a divergence of the orbital critical field and in a stabilization at low temperature of a cascade of superconducting phases separated by first order transistions. In this paper, we study the phase diagram as a function of the anisotropy. We discuss in details the experimental situation in the quasi-1D…
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