THEORY OF SUPERCONDUCTIVITY - NEW FORMULA FOR THE CRITICAL-TEMPERATURE

Based on the BCS Hamiltonian, the normal-to-super phase transition is investigated, approaching the critical temperature T(c) from the high temperature side. Non-zero momentum Cooper pairs, that is, pairs of electrons (holes) with antiparallel spins and nearly opposite momenta above T(c) in the bulk...

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Detalles Bibliográficos
Autores: FUJITA, S, KIMURA, T, ZHENG, Y, GODOY, S
Tipo de recurso: artículo
Estado:Versión publicada
Fecha de publicación:1992
País:México
Institución:Universidad Nacional Autónoma de México
Repositorio:Sistema de Información de la Facultad de Ciencias, UNAM
OAI Identifier:oai:repositorio.fciencias.unam.mx:11154/3511
Acceso en línea:http://hdl.handle.net/11154/3511
Access Level:acceso abierto
Palabra clave:Physics, Multidisciplinary
Descripción
Sumario:Based on the BCS Hamiltonian, the normal-to-super phase transition is investigated, approaching the critical temperature T(c) from the high temperature side. Non-zero momentum Cooper pairs, that is, pairs of electrons (holes) with antiparallel spins and nearly opposite momenta above T(c) in the bulk limit, are shown to move like free bosons with the energy (epsilon)-momentum (p) relation epsilon = 1/2nu(F)p, where nu(F) represents the Fermi velocity. The system of free Cooper pairs undergoes a phase transition of the second order at the critical temperature T(c) given by k(B)T(c) = 1.00856HBARnu(F)n1/3, where n is the number density of Cooper pairs. The ratio of the jump of the heat capacity, DELTAC, to the maximum heat capacity, C(s), is a universal constant: DELTAC/C(s) = 0.60874