Rhombohedral graphene multilayers host various broken-symmetry metallic phases as well as superconductors whose pairing mechanism and order parameter symmetry remain unsettled. Strikingly, experiments have revealed prominent new superconducting regions in rhombohedral bilayer and trilayer graphene devices with proximity-induced Ising spin-orbit coupling. We propose that these superconductors descend from a common spin-canted normal state that spontaneously breaks a U(1) spin symmetry and thus supports soft magnon modes. In particular, we show that these soft modes can mediate pairing through inter-band scattering events that are symmetry-forbidden in the absence of spin-orbit coupling, thus providing a promising explanation for spin-orbit-enabled pairing. Numerous other experimental observations -- including nontrivial dependence of superconductivity on the spin-orbit coupling strength, in-plane magnetic fields, and Fermi surface structure -- also naturally follow from our scenario.
@article{arxiv.2406.17036,
title = {Superconductivity from spin-canting fluctuations in rhombohedral graphene},
author = {Zhiyu Dong and Étienne Lantagne-Hurtubise and Jason Alicea},
journal= {arXiv preprint arXiv:2406.17036},
year = {2025}
}
Comments
Add an analysis on B-dependence of magnon gap and Tc