Spinodal decomposition in polarised Fermi superfluids

dc.creatorLamacraft, A.
dc.creatorMarchetti, F. M.
dc.date2007-01-28
dc.date2008-05-29
dc.date.accessioned2026-07-07T09:41:24Z
dc.date.available2026-07-07T09:41:24Z
dc.descriptionWe discuss the dynamics of phase separation through the process of spinodal decomposition in a Fermi superfluid with population imbalance. We discuss this instability first in terms of a phenomenological Landau theory. Working within the mean-field description at zero temperature, we then find the spinodal region in the phase diagram of polarisation versus interaction strength, and the spectrum of unstable modes in this region. After a quench, the spinodal decomposition starts from the Sarma state, which is a minimum of the free energy with respect to the order parameter at fixed density and polarisation and a maximum at fixed chemical potentials. The possibility of observing non-trivial domain structures in current experiments with trapped atomic gases is discussed.
dc.description6 pages, 3 eps figures (published version)
dc.identifierhttps://arxiv.org/abs/cond-mat/0701692
dc.identifierhttp://arxiv.org/abs/cond-mat/0701692
dc.identifierPhys. Rev. B 77, 014511 (2008)
dc.identifierdoi:10.1103/PhysRevB.77.014511
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/161814
dc.subjectSuperconductivity
dc.titleSpinodal decomposition in polarised Fermi superfluids
dc.typetext

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