Reentrant superconductivity in UTe
arXiv:2005.01074 · doi:10.1134/S0021364020120036
Abstract
The reentrant superconductivity is the peculiar phenomenon observed in paramagnetic metal UTe in magnetic field parallel to the hard magnetisation axis. It is difficult to explain it in terms of field dependent intensity of magnetic fluctuations like it is done for explanation of the formally similar phenomena in the ferromagnetic uranium superconductors URhGe, UCoGe. Extremely large initial slope of the upper critical field temperature dependence suggests that the phenomenon has the quasi-two-dimensional nature. Indeed, according to the recent band structure calculations by Yuanji Xu et al, Phys.Rev. Lett. {\bf 123}, 217002 (2019) the Fermi surface of UTe consists of two types slightly corrugated cylinders.The theory of reentrant superconductivity in UTe based on its quasi-two-dimensional structure is presented here.
7 pages, one Figure
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- Periodic Anderson model for magnetism and superconductivity in UTe2
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- Comparison of two superconducting phases induced by a magnetic field in UTe2
- Tuning magnetic confinement of spin-triplet superconductivity
- A review of UTe at high magnetic fields
- Enhanced triplet superconductivity in next generation ultraclean UTe2
- Expansion of the high field-boosted superconductivity in UTe2 under pressure
- Chiral Superconductivity in UTe via Emergent Symmetry and Spin Orbit Coupling
- Reentrant proximity-induced superconductivity for GeTe semimetal
- Reentrant orbital effect against superconductivity in the quasi-two-dimensional superconductor NbS
- Theory of Hofstadter Superconductors
- A Chiral Triplet Quasi-Two-Dimensional Superconductor in a Parallel Magnetic Field
- Reentrant Superconductivity from Competing Spin-Triplet Instabilities