Spontaneous symmetry breaking-induced thermospin effect in superconducting tunnel junctions
arXiv:2105.01527 · doi:10.1103/PhysRevB.104.184502
Abstract
We discuss the charge and the spin tunneling currents between two Bardeen-Cooper-Schrieffer (BCS) superconductors, where one density of states is spin-split. In the presence of a large temperature bias across the junction, we predict the generation of a spin-polarized thermoelectric current. This thermo-spin effect is the result of a spontaneous particle-hole symmetry breaking in the absence of a polarizing tunnel barrier. The two spin components, which move in opposite directions, generate a spin current larger than the purely polarized case when the thermo-active component dominates over the dissipative one.
References in corpus (15)
- The Josephson heat interferometer
- Nonlocal Thermoelectric Effects and Nonlocal Onsager Relations in a Three-Terminal Proximity-Coupled Superconductor-Ferromagnet Device
- Micrometre-scale refrigerators
- Revealing the magnetic proximity effect in EuS/Al bilayers through superconducting tunneling spectroscopy
- Superconductors as ideal spin sources for spintronics
- Thermopower induced by a supercurrent in superconductor-normal-metal structures
- Theory of a large thermoeffect in superconductors doped with magnetic impurities
- Coexistence of superconductivity and spin-splitting fields in superconductor/ferromagnetic insulator bilayers of arbitrary thickness
- Quantitative measurements of the thermal resistance of Andreev interferometers
- Phase-tunable thermoelectricity in a Josephson junction
- Nonlocal thermoelectricity in a topological Andreev interferometer
- Electron-hole imbalance and large thermoelectric effect in superconducting hybrids with spin-active interfaces
- Thermopower oscillations in mesoscopic Andreev interferometers
- Large thermoelectric effect in ballistic Andreev interferometers
- Superconducting double spin valve with extraordinary large tunable magnetoresistance