Field induced superconductivity with enhanced and tunable paramagnetic limit
arXiv:cond-mat/0505726 · doi:10.1103/PhysRevLett.95.167003
Abstract
We demonstrate that in a superconducting multilayered system with alternating interlayer coupling a new type of nonuniform superconducting state can be realized under in-plane magnetic field. The Zeeman effect in this state is compensated by the energy splitting between bonding and antibonding levels. Such compensation mechanism at low temperature leads to the field-induced superconductivity. We discuss the conditions for the experimental observation of the predicted phenomena.
5 pages, 4 figures included
References in corpus (2)
Cited by in corpus (8)
- Bosonization and density-matrix renormalization group studies of Fulde-Ferrell-Larkin-Ovchinnikov phase and irrational magnetization plateaus in coupled chains
- Recovering of superconductivity in exchange fields exceeding Pauli limiting field under spin-dependent quasiparticle distribution
- Orbital effect on intrinsic superconducting diode effect
- Re-entrant Fulde-Ferrell-Larkin-Ovchinnikov State in Small-Sized Superconductors
- Field-induced superconductivity mediated by odd-parity multipole fluctuation
- Field induced superconducting phase in Superconductor-Normal metal and Superconductor-Superconductor bilayer
- Interplay between orbital-quantization effects and the Fulde-Ferrell-Larkin-Ovchinnikov instability in multiple-band layered superconductors
- Field-induced topological pair-density wave states in a multilayer optical lattice