Generalized Cooper pairing and Bose-Einstein condensation
| dc.creator | Aguilera-Navarro, V. C. | |
| dc.creator | Fortes, M. | |
| dc.creator | de Llano, M. | |
| dc.date | 2003-06-30 | |
| dc.date.accessioned | 2026-07-07T02:52:07Z | |
| dc.date.available | 2026-07-07T02:52:07Z | |
| dc.description | A Bethe-Salpeter treatment of Cooper pairs (CPs) based on an ideal Fermi gas (IFG) "sea"' yields the familiar negative-energy, two-particle bound-state if two-hole CPs are ignored, but is meaningless otherwise as it gives purely-imaginary energies. However, when based on the BCS ground state, legitimate two-particle "moving" CPs emerge but as positive-energy, finite-lifetime resonances for nonzero center-of-mass momentum, with a \textit{linear}dispersion leading term. Bose-Einstein condensation of such pairs may thus occur in exactly two dimensions as it cannot with quadratic dispersion. | |
| dc.identifier | https://arxiv.org/abs/cond-mat/0306726 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/0306726 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/21717 | |
| dc.subject | Superconductivity | |
| dc.title | Generalized Cooper pairing and Bose-Einstein condensation | |
| dc.type | text |