Disorder Induced BCS–BEC Crossover in an Ultracold Fermi Gas

We develop the formalism for BCS–BEC crossover in the presence of weak random impurity and calculate the effect of the random potentials on the basic mean-field quantities. The disorder has been included through the Nozières and Schmitt–Rink theory of superconducting fluctuations, and we obtain the...

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Bibliographic Details
Published in:Journal of superconductivity and novel magnetism Vol. 26; no. 5; pp. 1891 - 1895
Main Authors: Khan, Ayan, Basu, Saurabh, Tanatar, B.
Format: Journal Article
Language:English
Published: Boston Springer US 01-05-2013
Springer
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Summary:We develop the formalism for BCS–BEC crossover in the presence of weak random impurity and calculate the effect of the random potentials on the basic mean-field quantities. The disorder has been included through the Nozières and Schmitt–Rink theory of superconducting fluctuations, and we obtain the disorder induced superfluid order parameter and chemical potential through a self-consistent calculation. We also calculate the condensate fraction which reveals a distinct nonmonotonic behavior. The downturn in the latter result occurs at the crossover regime with gradual depletion on the BEC side. The non-monotonic feature in the condensate fraction data has been measured in clean systems. Motivated by the above result, we discuss the stability of a disordered fermionic superfluid in the crossover regime.
ISSN:1557-1939
1557-1947
DOI:10.1007/s10948-012-1949-7