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.
- Received 13 October 2005
DOI:https://doi.org/10.1103/PhysRevB.73.052505
©2006 American Physical Society