Crystalline antiunitary symmetry in altermagnets selects pairing that produces robust nodal topological superconducting phases with Majorana flat bands and chiral edge states.
Su- perconducting states and intertwined orders in metallic alter- magnets
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cond-mat.supr-con 4years
2026 4verdicts
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D-wave altermagnets host a robust finite-temperature pair-density-wave superconducting phase driven by momentum-dependent spin splitting.
Altermagnetic spin splitting selects direction-selective triplet pairing in 2D d-wave metals and generates spin-locked Majorana edge states in both spin-conserving and Rashba-mixed regimes.
Pressure suppresses the density-wave feature in the d-wave altermagnet candidate CsV2Se2O and induces a reproducible, field-suppressible resistive downturn below 3 K suggestive of superconductivity.
citing papers explorer
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Nodal Topological Superconductivity Driven by Crystalline Antiunitary Symmetry in Altermagnets
Crystalline antiunitary symmetry in altermagnets selects pairing that produces robust nodal topological superconducting phases with Majorana flat bands and chiral edge states.
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Finite temperature pair density wave superconductivity in $d$-wave altermagnets
D-wave altermagnets host a robust finite-temperature pair-density-wave superconducting phase driven by momentum-dependent spin splitting.
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Direction-selective triplet pairing and spin-edge locking in altermagnetic metals
Altermagnetic spin splitting selects direction-selective triplet pairing in 2D d-wave metals and generates spin-locked Majorana edge states in both spin-conserving and Rashba-mixed regimes.
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Pressure-Induced Superconducting-like Transition in the $\it d$-wave Altermagnet Candidate CsV$_2$Se$_2$O
Pressure suppresses the density-wave feature in the d-wave altermagnet candidate CsV2Se2O and induces a reproducible, field-suppressible resistive downturn below 3 K suggestive of superconductivity.