Rise and fall of shape resonances in thin films of BCS superconductors
D. Valentinis, D. van der Marel, C. Berthod
DOI 10.1103/PhysRevB.94.054516 · Physical Review B
Active bibliographic source — not scientific approval
Bibliographic access preserves source history; it does not approve extracted materials or validate reported claims. Review warnings on each occurrence separately.
Abstract
The confinement of a superconductor in a thin film changes its Fermi-level density of states and is expected to change its critical temperature Tc. Previous calculations have reported large discontinuities of Tc when the chemical potential coincides with a subband edge. By solving the BCS gap equation exactly, we show that such discontinuities are artifacts and that Tc is a continuous function of the film thickness. We also find that Tc is reduced in thin films compared with the bulk if the confinement potential is lower than a critical value, while for stronger confinement Tc increases with decreasing film thickness, reaches a maximum, and eventually drops to zero. Our numerical results are supported by several exact solutions. We finally interpret experimental data for ultrathin lead thin films in terms of a thickness-dependent effective mass.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| Al Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Ga Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Sn Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| In Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Pb Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Bi Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| NbN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| FeSe Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| SrTiO3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
Similar papers
Shape resonances in the superconducting order parameter of ultrathin nanowires
similarity 0.95A. A. Shanenko & M. D. Croitoru
Source status unknown — claims are unverified
Oscillatory regimes of the thermomagnetic instability in superconducting films
similarity 0.95J. I. Vestgården et al.
Source status unknown — claims are unverified
Destruction of superconductivity in disordered materials: A dimensional crossover
similarity 0.95O. Crauste et al.
Source status unknown — claims are unverified
Effects of scattering on the field-induced Tc enhancement in thin superconducting films in a parallel magnetic field
similarity 0.95V. G. Kogan & R. Prozorov
Source status unknown — claims are unverified
Nonlinear response of diffusive superconductors to ac electromagnetic fields
similarity 0.95Pascal Derendorf et al.
Source status unknown — claims are unverified
Collective modes and their coupling to pair-breaking excitations in layered d-wave superconductors
similarity 0.95E. H. Hwang & S. Das Sarma
Source status unknown — claims are unverified