paper

Renormalization theory for the Fulde-Ferrell-Larkin-Ovchinnikov states at

arXiv:1706.01524 · doi:10.1103/PhysRevA.95.063626

Abstract

Within the renormalization group framework we study the stability of superfluid density wave states, known as Fulde-Ferrell-Larkin-Ovchinnikov (FFLO) phases, with respect to thermal order-parameter fluctuations in two and three-dimensional () systems. We analyze the renormalization-group flow of the relevant ordering wave-vector . The calculation indicates an instability of the FFLO-type states towards either a uniform superfluid or the normal state in and . In this is signaled by being renormalized towards zero, corresponding to the flow being attracted either to the usual Kosterlitz-Thouless fixed-point or to the normal phase. We supplement a solution of the RG flow equations by a simple scaling argument, supporting the generality of the result. The tendency to reduce the magnitude of by thermal fluctuations persists in , where the very presence of long-range order is immune to thermal fluctuations, but the effect of attracting towards zero by the flow remains observed at .

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