Anomalous specific heat jump in a two-component ultracold Fermi gas
arXiv:cond-mat/0605085 · doi:10.1103/PhysRevLett.97.140404
Abstract
The thermodynamic functions of a Fermi gas with spin population imbalance are studied in the temperature-asymmetry plane in the BCS limit. The low temperature domain is characterized by anomalous enhancement of the entropy and the specific heat above their values in the unpaired state, decrease of the gap and eventual unpairing phase transition as the temperature is lowered. The unpairing phase transition induces a second jump in the specific heat, which can be measured in calorimetric experiments. While the superfluid is unstable against a supercurrent carrying state, it may sustain a metastable state if cooled adiabatically down from the stable high-temperature domain. In the latter domain the temperature dependence of the gap and related functions is analogous to the predictions of the BCS theory.
4 pages, 3 figures. v2 includes a discussion of instabilities; v3: final version to appear in PRL
References in corpus (9)
- Observation of Phase Separation in a Strongly-Interacting Imbalanced Fermi Gas
- Phase diagram of a cold polarized Fermi gas
- Induced P-wave Superfluidity in Asymmetric Fermi Gases
- Surface Tension in Unitary Fermi Gases with Population Imbalance
- Stability conditions and Fermi surface topologies in a superconductor
- Realization and Detection of Fulde-Ferrell-Larkin-Ovchinnikov Superfluid Phases in Trapped Atomic Fermion Systems
- Breached Superfluidity via P-Wave Coupling
- Evaluating the phase diagram of superconductors with asymmetric spin populations
- Gapless phases of color-superconducting matter
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- Phase diagram of chiral quark matter: Fulde-Ferrell pairing from weak to strong coupling
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- A Mean Field Analysis of Pairing in Asymmetric Fermi Systems at Finite Temperature