Ubiquity of superconducting domes in BCS theory with finite-range potentials
arXiv:1810.03349 · doi:10.1103/PhysRevLett.122.157001
Abstract
Based on recent progress in mathematical physics, we present a reliable method to analytically solve the linearized BCS gap equation for a large class of finite-range interaction potentials leading to s-wave superconductivity. With this analysis, we demonstrate that the monotonic growth of the superconducting critical temperature with the carrier density, , predicted by standard BCS theory, is an artifact of the simplifying assumption that the interaction is quasi-local. In contrast, we show that any well-defined non-local potential leads to a "superconducting dome", i.e. a non-monotonic exhibiting a maximum value at finite doping and going to zero for large . This proves that, contrary to conventional wisdom, the presence of a superconducting dome is not necessarily an indication of competing orders, nor of exotic superconductivity. Our results provide a prototype example and guide towards improving ab-initio predictions of for real materials.
5 pages, 1 figure, + supplemental material
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Cited by in corpus (8)
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- Domes of in single-band and multiband superconductors with finite-range attractive interactions
- The BCS Critical Temperature at High Density
- The BCS Energy Gap at High Density
- Universality in low-dimensional BCS theory
- Universal and nonuniversal features of Bardeen-Cooper-Schrieffer theory with finite-range interactions
- High-Temperature Superconductivity from Finite-Range Attractive Interaction
- Finite-range effect in the two-dimensional density-induced BCS-BEC crossover