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VOLUME 59 (1994) | ISSUE 4 | PAGE 268
Strong-coupling corrections in a super-fluid Fermi gas with repulsion
Strong-coupling corrections to the coefficients β\—β^ are calculated for the quaternary terms in the Ginzburg-Landau free energy for a superfluid Fermi gas with repulsion. The stability conditions for the anisotropic A phase are analyzed. This theory is compared with the spin-fluctuation theory of Anderson, Brinkman, and Morel [Phys. Rev. 123, 1911 (1961); A 8, 2732 (1973)]. The possible realization of superfluid phases other than A and В is discussed.