Superconductivity from spin-canting fluctuations in rhombohedral graphene

TL;DR

This paper proposes that spin-canting fluctuations in rhombohedral graphene induce superconductivity by mediating pairing through soft magnon modes, explaining various experimental phenomena involving spin-orbit coupling and magnetic fields.

Contribution

It introduces a novel mechanism where spin-canted normal states support magnon-mediated pairing, linking spin fluctuations to superconductivity in rhombohedral graphene.

Findings

Soft magnon modes can mediate pairing in the presence of spin-orbit coupling.

Superconductivity depends on the strength of spin-orbit coupling and magnetic fields.

The proposed scenario explains experimental observations of superconductivity in rhombohedral graphene.

Abstract

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.