dc.contributor.author |
Varelogiannis, G |
en |
dc.contributor.author |
Moro, A |
en |
dc.date.accessioned |
2014-03-01T01:43:33Z |
|
dc.date.available |
2014-03-01T01:43:33Z |
|
dc.date.issued |
1995 |
en |
dc.identifier.uri |
https://dspace.lib.ntua.gr/xmlui/handle/123456789/24141 |
|
dc.relation.uri |
http://arxiv.org/abs/cond-mat/9511139 |
en |
dc.subject |
Electron Phonon Interaction |
en |
dc.subject |
high-tc superconductivity |
en |
dc.subject |
Superconductors |
en |
dc.title |
The gap symmetry is marginal in high-Tc superconductivity: Isotropic s-wave pairing leads to either s or d-wave gap depending on the Coulomb pseudopotential |
en |
heal.type |
journalArticle |
en |
heal.publicationDate |
1995 |
en |
heal.abstract |
We point out that in two-dimensional systems like high-$T_c$ superconductors,an isotropic s-wave electron-phonon interaction in the momentum decouplingregime leads to either s or d-wave superconductivity depending on theconventional values of the Coulomb pseudopotential. It is therefore possiblethat $YBa_2Cu_3O_7$ is an anisotropic d-wave and $Bi_2Sr_2CaCu_2O_8$ ananisotropic s-wave superconductor both having the same pairing interaction andsimilar |
en |