| Numéro |
J. Phys. IV France
Volume 03, Numéro C2, Juillet 1993
International Workshop on Electronic CrystalsECRYS - 93 |
|
|---|---|---|
| Page(s) | C2-311 - C2-314 | |
| DOI | https://doi.org/10.1051/jp4:1993263 | |
International Workshop on Electronic Crystals
ECRYS - 93
J. Phys. IV France 03 (1993) C2-311-C2-314
DOI: 10.1051/jp4:1993263
1 Laboratoire de Physique des Solides, Université Paris-Sud, 91405 Orsay, France
2 Science and Technology Center for Superconductivity, Argonne National Laboratory, Materials Science Division, Argonne IL 60439, U.S.A.
© EDP Sciences 1993
ECRYS - 93
J. Phys. IV France 03 (1993) C2-311-C2-314
DOI: 10.1051/jp4:1993263
Quasi-one-dimensional superconductors in strong magnetic field
N. DUPUIS1, G. MONTAMBAUX1 and C.A.R. SÁ DE MELO21 Laboratoire de Physique des Solides, Université Paris-Sud, 91405 Orsay, France
2 Science and Technology Center for Superconductivity, Argonne National Laboratory, Materials Science Division, Argonne IL 60439, U.S.A.
Abstract
We determine the phase diagram of a quasi-one-dimensional conductor (weakly coupled chains system with an open Fermi surface) in a magnetic field. The usual Ginzburg-Landau regime is followed, when the field is increased, by a cascade of superconducting phases separated by first order transitions, which ends with a strong reentrance of the superconducting phase. These new phases show a novel kind of symmetry of laminar type. The Zeeman splitting does not completely suppress the reentrance in very strong field, the ground state being in this case a Larkin-Ovchinnikov-Fulde-Ferrell state.
© EDP Sciences 1993