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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Published in: | Journal of superconductivity and novel magnetism Vol. 26; no. 5; pp. 1891 - 1895 |
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Main Authors: | , , |
Format: | Journal Article |
Language: | English |
Published: |
Boston
Springer US
01-05-2013
Springer |
Subjects: | |
Online Access: | Get full text |
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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. |
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ISSN: | 1557-1939 1557-1947 |
DOI: | 10.1007/s10948-012-1949-7 |