Orbital Effect for the Fulde-Ferrell-Larkin-Ovchinnikov Phase in a Quasi-Two-Dimensional Superconductor in a Parallel Magnetic Field

TL;DR

This paper theoretically investigates how orbital effects influence the FFLO superconducting phase in quasi-two-dimensional conductors under a parallel magnetic field, introducing a key parameter that characterizes the orbital suppression at zero temperature.

Contribution

It introduces a new parameter, $$, that quantifies the orbital effect's strength on the FFLO phase in Q2D superconductors at zero temperature.

Findings

The parameter $$ determines the orbital effect's impact on the FFLO phase.

Application of results to organic Q2D conductors shows relevance to experimental observations.

The study provides a theoretical framework for understanding orbital suppression in layered superconductors.

Abstract

We theoretically study the orbital destructive effect against superconductivity in a parallel magnetic field in the Fulde-Ferrell-Larkin-Ovchinnikov (FFLO or LOFF) phase at zero temperature in a quasi-two-dimensional (Q2D) conductor. We demonstrate that at zero temperature a special parameter, $\lambda = l_{\perp}(H)/d$, is responsible for strength of the orbital effect, where $l_{\perp}(H)$ is a typical "size" of the quasi-classical electron orbit in a magnetic field and $d$ is the inter-plane distance. We discuss applications of our results to the existing experiments on the FFLO phase in the organic Q2D conductors $\kappa$-(ET)$_2$Cu(NCS)$_2$ and $\kappa$-(ET)$_2$Cu[N(CN)$_2$]Cl.