{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:ZQT2ZHKBI4YLROKACVTXPB2MAN","short_pith_number":"pith:ZQT2ZHKB","schema_version":"1.0","canonical_sha256":"cc27ac9d414730b8b940156777874c03426181ed1d51c7dacf611ac230ca44d1","source":{"kind":"arxiv","id":"2601.19829","version":2},"attestation_state":"computed","paper":{"title":"Nonrelativistic-Ising superconductivity in p-wave magnets","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.supr-con","authors_text":"I. I. Mazin, Libor \\v{S}mejkal, Maxim Khodas","submitted_at":"2026-01-27T17:36:42Z","abstract_excerpt":"We discuss a possibility of superconductivity in the p-wave magnets. These are recently discovered materials that have zero net magnetization by symmetry and finite non-relativistic spin splitting of electron bands, like in altermagnets. Similarly, the spin polarizations is collinear in the momentum space. Yet, as opposed to altermagnets, the magnetization is noncollinear in the real space, and the spin splitting obeys time-reversal symmetry in the momentum space. As a result, if such material harbors superconductivity (due to phonons, or any other mechanism), the only supported superconductin"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2601.19829","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2026-01-27T17:36:42Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"df068b9532082e93dfbacfa9a4c41c784876c8d70c722ec8a6c54744ae55298c","abstract_canon_sha256":"2ac6da763353af626fcc3dc2d5523bbf55568d635d83caf03ce4e7520efa4813"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-08-14T00:39:33.134188Z","signature_b64":"FR+yW+oHPeppnBVACmHhgwjOzfrr/9oDVXItdcJeZC+Dokk2dIUKiRsG/b9NAAKvvSYPhXXkmVl8fxERZljxAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cc27ac9d414730b8b940156777874c03426181ed1d51c7dacf611ac230ca44d1","last_reissued_at":"2026-08-14T00:39:33.127738Z","signature_status":"signed_v1","first_computed_at":"2026-08-14T00:39:33.127738Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nonrelativistic-Ising superconductivity in p-wave magnets","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.supr-con","authors_text":"I. I. Mazin, Libor \\v{S}mejkal, Maxim Khodas","submitted_at":"2026-01-27T17:36:42Z","abstract_excerpt":"We discuss a possibility of superconductivity in the p-wave magnets. These are recently discovered materials that have zero net magnetization by symmetry and finite non-relativistic spin splitting of electron bands, like in altermagnets. Similarly, the spin polarizations is collinear in the momentum space. Yet, as opposed to altermagnets, the magnetization is noncollinear in the real space, and the spin splitting obeys time-reversal symmetry in the momentum space. As a result, if such material harbors superconductivity (due to phonons, or any other mechanism), the only supported superconductin"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2601.19829","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2601.19829/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2601.19829","created_at":"2026-08-14T00:39:33.132599+00:00"},{"alias_kind":"arxiv_version","alias_value":"2601.19829v2","created_at":"2026-08-14T00:39:33.132599+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2601.19829","created_at":"2026-08-14T00:39:33.132599+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZQT2ZHKBI4YL","created_at":"2026-08-14T00:39:33.132599+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZQT2ZHKBI4YLROKA","created_at":"2026-08-14T00:39:33.132599+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZQT2ZHKB","created_at":"2026-08-14T00:39:33.132599+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":6,"internal_anchor_count":6,"sample":[{"citing_arxiv_id":"2606.31867","citing_title":"Giant perpendicular Edelstein polarization in 2D compensated magnets via bichromatic Floquet driving","ref_index":54,"is_internal_anchor":true},{"citing_arxiv_id":"2605.28391","citing_title":"Global magnetic phase diagram and multiple unconventional magnets in NiAs-type compounds","ref_index":74,"is_internal_anchor":true},{"citing_arxiv_id":"2605.17649","citing_title":"Competition and coexistence of superconducting symmetries in $p$-wave magnets","ref_index":20,"is_internal_anchor":true},{"citing_arxiv_id":"2603.22243","citing_title":"Supercurrent-Driven N\\'eel Torque in Superconductor/Altermagnet Hybrids","ref_index":16,"is_internal_anchor":true},{"citing_arxiv_id":"2605.01686","citing_title":"Topological Ising superconductivity in two-dimensional p-wave magnet","ref_index":36,"is_internal_anchor":true},{"citing_arxiv_id":"2604.18695","citing_title":"$P$-wave Orbital Magnetism","ref_index":39,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZQT2ZHKBI4YLROKACVTXPB2MAN","json":"https://pith.science/pith/ZQT2ZHKBI4YLROKACVTXPB2MAN.json","graph_json":"https://pith.science/api/pith-number/ZQT2ZHKBI4YLROKACVTXPB2MAN/graph.json","events_json":"https://pith.science/api/pith-number/ZQT2ZHKBI4YLROKACVTXPB2MAN/events.json","paper":"https://pith.science/paper/ZQT2ZHKB"},"agent_actions":{"view_html":"https://pith.science/pith/ZQT2ZHKBI4YLROKACVTXPB2MAN","download_json":"https://pith.science/pith/ZQT2ZHKBI4YLROKACVTXPB2MAN.json","view_paper":"https://pith.science/paper/ZQT2ZHKB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2601.19829&json=true","fetch_graph":"https://pith.science/api/pith-number/ZQT2ZHKBI4YLROKACVTXPB2MAN/graph.json","fetch_events":"https://pith.science/api/pith-number/ZQT2ZHKBI4YLROKACVTXPB2MAN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZQT2ZHKBI4YLROKACVTXPB2MAN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZQT2ZHKBI4YLROKACVTXPB2MAN/action/storage_attestation","attest_author":"https://pith.science/pith/ZQT2ZHKBI4YLROKACVTXPB2MAN/action/author_attestation","sign_citation":"https://pith.science/pith/ZQT2ZHKBI4YLROKACVTXPB2MAN/action/citation_signature","submit_replication":"https://pith.science/pith/ZQT2ZHKBI4YLROKACVTXPB2MAN/action/replication_record"}},"created_at":"2026-08-14T00:39:33.132599+00:00","updated_at":"2026-08-14T00:39:33.132599+00:00"}