Strong-coupling Properties of a -wave Interacting Fermi Gas on the Viewpoint of Specific Heat at Constant Volume
arXiv:1610.08598 · doi:10.7566/JPSJ.86.024302
Abstract
We theoretically investigate the specific heat at constant volume in the normal state of a -wave interacting Fermi gas. Including fluctuations in the -wave Cooper channel within the framework of the strong-coupling theory developed by Nozières and Schmitt-Rink, we clarify how as a function of temperature varies, as one moves from the weak-coupling regime to the strong-coupling limit. In the weak-coupling regime, is shown to be enhanced by -wave pairing fluctuations, near the superfluid phase transition temperature . Similar enhancement of is also obtained in the strong-coupling regime, which, however, reflects that system is close an ideal Bose gas of -wave two-body bound molecules. Using these results, we classify the normal state into (1) the normal Fermi gas regime, (2) the -wave molecular Bose gas regime, and (3) the region between the two, where -wave pairing fluctuations are dominant. Since the current experiments can only access the normal phase of a -wave interacting Fermi gas, our results would be useful for experiments to understand strong-coupling properties of this Fermi system above .
7 pages, 6 figures
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