Anharmonic theory of superconductivity in the high-pressure materials
arXiv:2007.04981 · doi:10.1103/PhysRevB.103.094519
Abstract
Electron-phonon superconductors at high pressures have displayed the highest values of critical superconducting temperature on record, now rapidly approaching room temperature. Despite the importance of high- superconductivity in the quest for room-temperature superconductors, a mechanistic understanding of the effect of pressure and its complex interplay with phonon anharmonicity and superconductivity is missing, as numerical simulations can only bring system-specific details clouding out key players controlling the physics. Here we develop a minimal model of electron-phonon superconductivity under an applied pressure which takes into account the anharmonic decoherence of the optical phonons. We find that behaves non-monotonically as a function of the ratio , where is the optical phonon damping and the optical phonon energy at zero pressure and momentum. Optimal pairing occurs for a critical ratio when the phonons are on the verge of decoherence ("diffuson-like" limit). Our framework gives insights into recent experimental observations of as a function of pressure in the complex BCS material TlInTe.
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- Turning non-superconducting elements into superconductors by quantum confinement and proximity
- Estimation of Grüneisen parameter of high-entropy-alloy-type functional materials
- Pressure-induced concurrent amorphization and superconductivity in topological material NbNiTe5