Upper critical field as a probe for multiband superconductivity in bulk and interfacial STO
arXiv:1401.5318 · doi:10.1007/s10948-015-3052-3
Abstract
We investigate the temperature dependence of the upper critical field as a tool to probe the possible presence of multiband superconductivity at the interface of LAO/STO. The behaviour of can clearly indicate two-band superconductivity through its nontrivial temperature dependence. For the disorder scattering dominated two-dimensional LAO/STO interface we find a characteristic non-monotonic curvature of the . We also analyse the for multiband bulk STO and find similar behaviour.
17 pages, 10 figures
References in corpus (5)
- Electric Field Control of the LaAlO/SrTiO Interface Ground State
- Very High Field Two-Band Superconductivity in LaFeAsO_0.89F_0.11
- High mobility conduction at (110) and (111) LaAlO3/SrTiO3 interfaces
- Critical doping for the onset of a two-band superconducting ground state in SrTiO
- A review of two-band superconductivity: materials and effects on the thermodynamic and reversible mixed-state properties
Cited by in corpus (11)
- Superconductivity in dilute SrTiO: a review
- Possible signatures of mixed-parity superconductivity in doped polar SrTiO3 films
- Unconventional multi-band superconductivity in bulk SrTiO and LaAlO/SrTiO interfaces
- Multiorbital Ferroelectric Superconductivity in doped SrTiO3
- Impact of disorder on the superconducting transition temperature near a Lifshitz transition
- Upper critical magnetic field and multiband superconductivity in artificial high-Tc superlattices of nano quantum wells
- Ferroelectricity-induced multiorbital odd-frequency superconductivity in SrTiO
- Magnetic behaviour of dirty multiband superconductors near the upper critical field
- Effects of paramagnetic pair-breaking and spin-orbital coupling on multi-band superconductivity
- Two-gap superconductivity in the noncentrosymmetric LaSe compound
- High magnetic field response of superconductivity dome in quantum artificial High Tc superlattices with variable geometry