Published March 12, 2026 | Version Published
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Superconductivity from Spin-Canting Fluctuations in Rhombohedral Graphene

  • 1. ROR icon California Institute of Technology
  • 2. ROR icon Université de Sherbrooke

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 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 interband 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.

Copyright and License

Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license.  Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI.

Acknowledgement

We are grateful to Trevor Arp, Erez Berg, Nick Bultinck, Andrey Chubukov, Julian Ingham, Long Ju, Hyunjin Kim, Patrick Lee, Leonid Levitov, Cyprian Lewandowski, Stevan Nadj-Perge, Caitlin Patterson, Gal Shavit, Owen Sheekey, Tomohiro Soejima, Alex Thomson, Yaar Vituri, Andrea Young, and Yiran Zhang for insightful discussions. We want to thank Alex Thomson and Johnson Guanyao Chen for pointing out a mistake in the previous version of this manuscript, where we obtained an intraband two-magnon pairing interaction involving intermediate electrons away from the Fermi surfaces that diverged as 𝑞 →0. This divergence is, in fact, canceled by higher-order terms in the magnon-fermion coupling [59]. 

Funding

Z. D. and É. L.-H. were supported by the Gordon and Betty Moore Foundation’s EPiQS Initiative, Grant No. GBMF8682. Portions of this work were supported by the U.S. Department of Energy, Office of Science, National Quantum Information Science Research Centers, Quantum Science Center (derivation of magnon spectrum and magnon-mediated interactions, J. A.). Additional support was provided by the Caltech Institute for Quantum Information and Matter, a National Science Foundation (NSF) Physics Frontiers Center (NSF Grant No. PHY-2317110).

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Additional details

Related works

Is new version of
Discussion Paper: arXiv:2406.17036 (arXiv)

Funding

Gordon and Betty Moore Foundation
GBMF8682
United States Department of Energy
National Quantum Information Science Research Centers
Quantum Science Center
Caltech Institute for Quantum Information and Matter
National Science Foundation
PHY-2317110

Dates

Submitted
2024-07-22
Accepted
2026-02-12