The BCS gap equation for spin-polarized fermions
arXiv:1107.0405 · doi:10.1063/1.3670747
Abstract
We study the BCS gap equation for a Fermi gas with unequal population of spin-up and spin-down states. For , with the temperature and the chemical potential difference, the question of existence of non-trivial solutions can be reduced to spectral properties of a linear operator, similar to the unpolarized case studied previously in \cite{FHNS,HHSS,HS}. For the phase diagram is more complicated, however. We derive upper and lower bounds for the critical temperature, and study their behavior in the small coupling limit.
23 pages, 1 figure
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- Microscopic Derivation of Ginzburg-Landau Theory and the BCS Critical Temperature Shift in General External Fields
- Another operator-theoretical proof for the second-order phase transition in the BCS-Bogoliubov model of superconductivity
- An operator-theoretical study of the specific heat and the critical magnetic field in the BCS-Bogoliubov model of superconductivity
- A lower bound for the BCS functional with boundary conditions at infinity
- An operator-theoretical study on the BCS-Bogoliubov model of superconductivity near absolute zero temperature
- Linear Criterion for an Upper Bound on the Bardeen-Cooper-Schrieffer Critical Temperature