pith:2TRXTL4E
Nodal Topological Superconductivity Driven by Crystalline Antiunitary Symmetry in Altermagnets
Crystalline antiunitary symmetry in fourfold altermagnets forbids pure spin-singlet pairing and selects structures yielding emergent chiral symmetries that produce nodal topological superconductivity.
arxiv:2605.13656 v1 · 2026-05-13 · cond-mat.supr-con
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Claims
the native crystalline antiunitary symmetry T C4z generically forbids pure spin-singlet pairing and selects pairing structures that admit Bogoliubov-de Gennes (BdG) Hamiltonians with emergent chiral symmetries. These symmetries further give rise to robust nodal topological phases over broad parameter regimes, including a nodal-point phase hosting Majorana flat bands (MFBs) and two distinct nodal-loop phases with chiral Majorana edge states.
That the dominant pairing interaction in real fourfold altermagnets falls into the symmetry-selected channels that produce the emergent chiral symmetries, without being overwhelmed by competing orders or other pairing symmetries.
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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| First computed | 2026-05-18T02:44:17.391135Z |
|---|---|
| Builder | pith-number-builder-2026-05-17-v1 |
| Signature | Pith Ed25519
(pith-v1-2026-05) · public key |
| Schema | pith-number/v1.0 |
Canonical hash
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· · · · ·Agent API
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curl -sH 'Accept: application/ld+json' https://pith.science/pith/2TRXTL4EYHNUOA4D4KZIWCR3QA \
| jq -c '.canonical_record' \
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Canonical record JSON
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