Strong electron correlations in Sr2RuO4 produce unconventional plasmon dispersion, intrinsic width below the electron-hole continuum, and a high-energy peak from incoherent transitions.
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Mean-field theory on a quartic-dispersion Chern band for rhombohedral graphene yields a chiral topological superconductor that transitions to a trivial BEC at T=0; the composite-fermion version realizes a Moore-Read state.
Vacuum fluctuations of magnetic flux in an LC resonator mediate electron pairing in 2D systems to form a pair-density wave topological chiral superconductor with Tc of several Kelvin or higher.
Sr2RuO4 exhibits reversed anisotropy in Andreev bound states, pointing to inter-orbital superconducting pairing that generates surface states while suppressing edge modes.
citing papers explorer
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Unconventional plasmon dynamics due to strong correlations in Sr$_2$RuO$_4$
Strong electron correlations in Sr2RuO4 produce unconventional plasmon dispersion, intrinsic width below the electron-hole continuum, and a high-energy peak from incoherent transitions.
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Chiral superconductivity from parent Chern band and its non-Abelian generalization
Mean-field theory on a quartic-dispersion Chern band for rhombohedral graphene yields a chiral topological superconductor that transitions to a trivial BEC at T=0; the composite-fermion version realizes a Moore-Read state.
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Chiral electron-fluxon superconductivity in circuit quantum magnetostatics
Vacuum fluctuations of magnetic flux in an LC resonator mediate electron pairing in 2D systems to form a pair-density wave topological chiral superconductor with Tc of several Kelvin or higher.
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Directional Andreev-Reflection Signatures of Inter-Orbital Pairing in Sr$_2$RuO$_4$
Sr2RuO4 exhibits reversed anisotropy in Andreev bound states, pointing to inter-orbital superconducting pairing that generates surface states while suppressing edge modes.