Superconductivity in rhombohedral trilayer graphene is explained as quasiparticle pairing from the intervalley coherent state, producing Tc proportional to epsilon_D exp(-2 over rho_qp U) and coherence length xi approximately v over sqrt(mu Tc) that match data.
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Reviews the FL* theory for cuprates using ancilla layer models and SU(2) gauge theories to explain pseudogap hole pockets of area p/8, Fermi arcs, and transitions to d-wave superconductivity and Fermi liquid behavior.
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Superconductivity from Quasiparticle Pairing of Intervalley Coherent State in Rhombohedral Trilayer Graphene
Superconductivity in rhombohedral trilayer graphene is explained as quasiparticle pairing from the intervalley coherent state, producing Tc proportional to epsilon_D exp(-2 over rho_qp U) and coherence length xi approximately v over sqrt(mu Tc) that match data.
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Fractionalized Fermi liquids and the cuprate phase diagram
Reviews the FL* theory for cuprates using ancilla layer models and SU(2) gauge theories to explain pseudogap hole pockets of area p/8, Fermi arcs, and transitions to d-wave superconductivity and Fermi liquid behavior.