Superconductor-insulator transition in Coulomb disorder
arXiv:0708.2516 · doi:10.1103/PhysRevB.76.224511
Abstract
Superconductor-insulator transition driven by the decreasing concentration of electrons is studied in the case of the disorder potential created by randomly positioned charged impurities. Electrons and Cooper pairs (formed by an non-Coulomb attraction) nonlinearly screen the random potential of impurities. Both electrons and Cooper pairs can be delocalized or localized in the resulting self-consistent potential. The border separating the superconductor and insulator phases in the plane of the concentration of electrons and the length of the Cooper pair is found. For a strong disorder the central segment of this border follows the BEC-BCS crossover line defined for a clean sample.
4.5 pages, introduction rewritten, a dozen of references added, 2D case added
References in corpus (7)
- Nature of the superconductor-insulator transition in disordered superconductors
- Role of Spatial Amplitude Fluctuations in Highly Disordered s-Wave Superconductors
- Dissipation effects on the superconductor-insulator transition in 2-D superconductors
- Evidence for charge Kondo effect in superconducting Tl-doped PbTe
- Electrostatic Tuning of the Superconductor-Insulator Transition in Two Dimensions
- Superconductivity in charge Kondo systems
- Quantum Metallicity on the High-Field Side of the Superconductor-Insulator Transition
Cited by in corpus (5)
- Localization and Superconductivity in Doped Semiconductors
- Localization of disordered bosons and magnets in random fields
- Compensation driven superconductor-insulator transition
- Superfluid Bloch dynamics in an incommensurate lattice
- Anderson localization on the Falicov-Kimball model with Coulomb disorder