Ginzburg-Landau theory of superconducting surfaces under electric fields
arXiv:cond-mat/0511364 · doi:10.1103/PhysRevB.73.052505
Abstract
A boundary condition for the Ginzburg-Landau wave function at surfaces biased by a strong electric field is derived within the de Gennes approach. This condition provides a simple theory of the field effect on the critical temperature of superconducting layers.
4 pages, 1 figure