Quantifying nonadiabaticity in major families of superconductors

E. F. Talantsev

doi:10.3390/nano13010071

paper

Quantifying nonadiabaticity in major families of superconductors

arXiv:2212.02396 · doi:10.3390/nano13010071

Abstract

The classical Bardeen-Cooper-Schrieffer and Eliashberg theories of the electron-phonon-mediated superconductivity are based on the Migdal theorem, which is an assumption that the energy of charge carriers, $k_{B} T_{F}$ , significantly exceeds the phononic energy, $ℏ ω_{D}$ , of the crystalline lattice. This assumption, which is also known as adiabatic approximation, implies that the superconductor exhibits fast charge carriers and slow phonons. This picture is valid for pure metals and metallic alloys because these superconductors exhibit $ℏ ω_{D}$ / $k_{B} T_{F} < 0.01$ . However, n-type doped semiconducting $S r T i O_{3}$ was the first superconductor which beyond this adiabatic approximation, because this material exhibits $ℏ ω_{D}$ / $k_{B} T_{F}$ ~ $50$ . There is growing number of newly discovered superconductors which also beyond the adiabatic approximation. Here, leaving apart pure theoretical aspects of nonadiabatic superconductors, we classified major classes of superconductors (including, elements, A-15 and Heusler alloys, Laves phases, intermetallics, noncentrosymmetric compounds, cuprates, pnictides, highly-compressed hydrides and oxygen, and magic-angle twisted bilayer graphene) by the strength of nonadiabaticity (for which the ratio of the Debye temperature to the Fermi temperature, $T_{θ} / T_{F}$ , is used as a criterion for the nonadiabaticity) versus the superconducting transition temperature, $T_{c}$ . The discussion of this classification scheme and its relation to other known classification counterparts is given.

arXiv comment22 pages, 3 figures, 1 table

Quantifying nonadiabaticity in major families of superconductors

Abstract

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