A realistic 12-orbital Dirac-Anderson model of CeRh2As2 shows that quantum-geometric magnetic monopole fluctuations from the M-point Dirac point lead to nearly degenerate B1u and B2g spin-triplet superconducting instabilities.
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Quantum geometric magnetic monopole and two-phase superconductivity in CeRh$_2$As$_2$
A realistic 12-orbital Dirac-Anderson model of CeRh2As2 shows that quantum-geometric magnetic monopole fluctuations from the M-point Dirac point lead to nearly degenerate B1u and B2g spin-triplet superconducting instabilities.