Strong Coupling Effects on the Specific Heat of an Ultracold Fermi Gas in the Unitarity Limit
arXiv:1507.06403 · doi:10.1007/s10909-015-1387-6
Abstract
We investigate strong-coupling corrections to the specific heat in the normal state of an ultracold Fermi gas in the BCS-BEC crossover region. A recent experiment on a Li unitary Fermi gas [M. J. H. Ku, {\it et. al.}, Science {\bf 335}, 563 (2012)] shows that is remarkably amplified near the superfluid phase transition temperature , being similar to the well-known -structure observed in liquid He. Including pairing fluctuations within the framework of the strong-coupling theory developed by Nozières and Schmitt-Rink, we show that strong pairing fluctuations are sufficient to explain the anomalous behavior of observed in a Li unitary Fermi gas near . We also show that there is no contribution from {\it stable} preformed Cooper pairs to at the unitarity. This indicates that the origin of the observed anomaly is fundamentally different from the case of liquid He, where {\it stable} He Bose atoms induce the -structure in near the superfluid instability. Instead, the origin is the suppression of the entropy , near , due to the increase of {\it metastable} preformed Cooper pairs. Our results indicate that the specific heat is a useful quantity to study the effects of pairing fluctuations on the thermodynamic properties of an ultracold Fermi gas in the BCS-BEC crossover region.
7 pages, 3 figures
References in corpus (8)
- Vortices and Superfluidity in a Strongly Interacting Fermi Gas
- Revealing the Superfluid Lambda Transition in the Universal Thermodynamics of a Unitary Fermi Gas
- Collective excitations of a degenerate gas at the BEC-BCS crossover
- Thermodynamics of the BCS-BEC crossover
- Thermodynamic Measurements in a Strongly Interacting Fermi Gas
- Evolution of the Normal State of a Strongly Interacting Fermi Gas from a Pseudogap Phase to a Molecular Bose Gas
- Comparative study of strong coupling theories of a trapped Fermi gas at unitarity
- Temperature of a trapped unitary Fermi gas at finite entropy