Many-body perturbation theory for the superconducting quantum dot: Fundamental role of the magnetic field

0553383 - FZÚ 2022 RIV US eng J - Článek v odborném periodiku
Janiš, Václav - Yan, Jiawei
Many-body perturbation theory for the superconducting quantum dot: Fundamental role of the magnetic field.
Physical Review B. Roč. 103, č. 23 (2021), č. článku 235163. ISSN 2469-9950. E-ISSN 2469-9969
Grant CEP: GA ČR GA19-13525S; GA MŠMT LTC19045
Institucionální podpora: RVO:68378271
Klíčová slova: quantum dot * superconductivity * Andreev bound states * perturbation theory * magnetic field * 0-pi transition * atomic limit
Obor OECD: Condensed matter physics (including formerly solid state physics, supercond.)
Impakt faktor: 3.908, rok: 2021
Způsob publikování: Omezený přístup
https://doi.org/10.1103/PhysRevB.103.235163

We develop the general many-body perturbation theory for a superconducting quantum dot represented by a single-impurity Anderson model attached to superconducting leads. We build our approach on a thermodynamically consistent mean-field approximation with a two-particle self-consistency of the parquet type. The two-particle self-consistency leading to a screening of the bare interaction proves substantial for suppressing the spurious transitions of the Hartree-Fock solution. We demonstrate that the magnetic field plays a fundamental role in the extension of the perturbation theory beyond the weakly correlated 0 phase. It controls the critical behavior of the 0-pi quantum transition and lifts the degeneracy in the pi phase, where the limits to zero temperature and zero magnetic field do not commute. The response to the magnetic field is quite different in 0 and pi phases. While the magnetic susceptibility vanishes in the 0 phase it becomes divergent in the pi phase at zero temperature.
Trvalý link: http://hdl.handle.net/11104/0328338