Enhanced Superconductivity at a Corner for the Linear BCS Equation
arXiv:2308.07115 · doi:10.1017/fms.2024.145
Abstract
We consider the critical temperature for superconductivity, defined via the linear BCS equation. We prove that at weak coupling the critical temperature for a sample confined to a quadrant in two dimensions is strictly larger than the one for a half-space, which in turn is strictly larger than the one for . Furthermore, we prove that the relative difference of the critical temperatures vanishes in the weak coupling limit.
arXiv comment36 pages, 1 figure; published version
References in corpus (12)
- The BCS Functional for General Pair Interactions
- The BCS functional of superconductivity and its mathematical properties
- Boundary states with elevated critical temperatures in Bardeen-Cooper-Schrieffer superconductors
- Microscopic derivation of superconductor-insulator boundary conditions for Ginzburg-Landau theory revisited. Enhanced superconductivity at boundaries with and without magnetic field
- Boundary effects in two-band superconductors
- Boundary Superconductivity in the BCS Model
- The BCS critical temperature in a weak homogeneous magnetic field
- Universality in low-dimensional BCS theory
- Microscopic Derivation of Ginzburg-Landau Theory and the BCS Critical Temperature Shift in a Weak Homogeneous Magnetic Field
- Microscopic Derivation of Ginzburg-Landau Theory and the BCS Critical Temperature Shift in General External Fields
- Linear Criterion for an Upper Bound on the Bardeen-Cooper-Schrieffer Critical Temperature
- On the Ginzburg-Landau Energy of Corners