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Superconductivity from spin-canting fluctuations in rhombohedral graphene
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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.
Forward citations
Cited by 4 Pith papers
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Superconductivity via paramagnon and magnon exchange in a 2D near-ferromagnetic full metal and ferromagnetic half-metal
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Superconductivity induced by spin-orbit coupling in a two-valley ferromagnet
In a canted ferromagnet with Ising spin-orbit coupling, two-magnon processes generate an attractive, SOC-induced pairing interaction that may drive superconductivity despite static repulsion.
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Spontaneous vortex lattice due to orbital magnetization in valley polarized superconductors
The paper predicts that orbital magnetization in valley-polarized superconductors can spontaneously create a vortex lattice, with a concrete estimate for rhombohedral graphene.
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Magnon-Mediated Superconductivity in a 2D Itinerant Ferromagnet with Weak Easy-plane Magnetic Anisotropy
Weak easy-plane anisotropy generates attractive equal-spin p-wave pairing via two-magnon exchange in a 2D half-metal, with λp enhanced to O(1) near the ferromagnetic onset.
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