Phase diagram of strongly-coupled Rashba systems

Abstract Motivated by the recent discovery of a possible field-mediated parity switch within the superconducting state of CeRh 2 As 2 (Khim et al 2021 Science 373 1012), we thoroughly investigate the dependence of the superconducting state of a strongly-coupled Rashba mono- and bilayer on internal parameters and an applied magnetic field. The role of interlayer pairing, spin orbit coupling, doping rate and applied magnetic field and their interplay was examined numerically at low temperature within a t-J- like model, uncovering complex phase diagrams and transitions between superconducting states with different symmetry.

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Publication Details

Journal
New Journal of Physics
Published
2024-09-01
DOI
https://doi.org/10.1088/1367-2630/ad7630
Citations
2
Primary Topic
Physics of Superconductivity and Magnetism
Type
article
Field-Weighted Citation Impact
0.62
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article

Phase diagram of strongly-coupled Rashba systems

P. M. R. Brydon, Brianna K. Nally
2 citations
New Journal of Physics
Physics of Superconductivity and Magnetism
0.62
article

Phase diagram of strongly-coupled Rashba systems

P. M. R. Brydon, Brianna K. Nally
article en
2 citations

Abstract

Abstract Motivated by the recent discovery of a possible field-mediated parity switch within the superconducting state of CeRh 2 As 2 (Khim et al 2021 Science 373 1012), we thoroughly investigate the dependence of the superconducting state of a strongly-coupled Rashba mono- and bilayer on internal parameters and an applied magnetic field. The role of interlayer pairing, spin orbit coupling, doping rate and applied magnetic field and their interplay was examined numerically at low temperature within a t-J- like model, uncovering complex phase diagrams and transitions between superconducting states with different symmetry.

New Journal of PhysicsVol. 26(9)
University of Otago (NZ), MacDiarmid Institute for Advanced Materials and Nanotechnology (NZ)
Openalex Percentile: Top 34%
Physics of Superconductivity and Magnetism
0.62
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