{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:SL64ZBHICLRHVT7ISI77WQWKAW","short_pith_number":"pith:SL64ZBHI","schema_version":"1.0","canonical_sha256":"92fdcc84e812e27acfe8923ffb42ca05b882e2b12fd0e115a2189a65c33bf48f","source":{"kind":"arxiv","id":"2602.23986","version":2},"attestation_state":"computed","paper":{"title":"Quantum spin models of commensurate $p$-wave magnets","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"Gibaik Sim, Stephan Rachel","submitted_at":"2026-02-27T13:03:44Z","abstract_excerpt":"The $p$-wave magnet has emerged as a new type of magnetism exhibiting odd-parity, time-reversal-symmetric spin splitting in momentum space, and has attracted considerable interest as a promising platform for spintronic applications. However, the theoretical understanding of the fundamental mechanism responsible for stabilizing this phase remains limited. In this work, we identify a microscopic interacting model that realizes the $p$-wave magnet as its ground state. We first introduce a Hubbard model and derive the corresponding low-energy spin Hamiltonian. At the classical level, we find that "},"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":"2602.23986","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2026-02-27T13:03:44Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"f15fe9839c3e87819e3a7a5accf005018379467d570d5cfb5429a0d9dfc0d7f1","abstract_canon_sha256":"e97c691e0e69472e13ab7c4c112a43f361501cccafc25862133a518254405c23"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-08T01:19:11.159871Z","signature_b64":"NRfca9qZ06uFPmSfmundapaF7A5HYwWOCpKtwCmjXLuUfu1vVBCIOqkyXXP0oRM6SqsQSAa2HwFh4q0lfqWuBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"92fdcc84e812e27acfe8923ffb42ca05b882e2b12fd0e115a2189a65c33bf48f","last_reissued_at":"2026-07-08T01:19:11.159278Z","signature_status":"signed_v1","first_computed_at":"2026-07-08T01:19:11.159278Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum spin models of commensurate $p$-wave magnets","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"Gibaik Sim, Stephan Rachel","submitted_at":"2026-02-27T13:03:44Z","abstract_excerpt":"The $p$-wave magnet has emerged as a new type of magnetism exhibiting odd-parity, time-reversal-symmetric spin splitting in momentum space, and has attracted considerable interest as a promising platform for spintronic applications. However, the theoretical understanding of the fundamental mechanism responsible for stabilizing this phase remains limited. In this work, we identify a microscopic interacting model that realizes the $p$-wave magnet as its ground state. We first introduce a Hubbard model and derive the corresponding low-energy spin Hamiltonian. At the classical level, we find that "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2602.23986","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/2602.23986/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":"2602.23986","created_at":"2026-07-08T01:19:11.159348+00:00"},{"alias_kind":"arxiv_version","alias_value":"2602.23986v2","created_at":"2026-07-08T01:19:11.159348+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2602.23986","created_at":"2026-07-08T01:19:11.159348+00:00"},{"alias_kind":"pith_short_12","alias_value":"SL64ZBHICLRH","created_at":"2026-07-08T01:19:11.159348+00:00"},{"alias_kind":"pith_short_16","alias_value":"SL64ZBHICLRHVT7I","created_at":"2026-07-08T01:19:11.159348+00:00"},{"alias_kind":"pith_short_8","alias_value":"SL64ZBHI","created_at":"2026-07-08T01:19:11.159348+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":4,"sample":[{"citing_arxiv_id":"2606.26222","citing_title":"The fate of odd-parity magnetism in one dimension","ref_index":16,"is_internal_anchor":true},{"citing_arxiv_id":"2606.23806","citing_title":"Nonrelativistic Spin-Orbit-Coupling Effects in Odd-Parity Coplanar Magnets","ref_index":61,"is_internal_anchor":true},{"citing_arxiv_id":"2605.01686","citing_title":"Topological Ising superconductivity in two-dimensional p-wave magnet","ref_index":31,"is_internal_anchor":true},{"citing_arxiv_id":"2604.18695","citing_title":"$P$-wave Orbital Magnetism","ref_index":27,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/SL64ZBHICLRHVT7ISI77WQWKAW","json":"https://pith.science/pith/SL64ZBHICLRHVT7ISI77WQWKAW.json","graph_json":"https://pith.science/api/pith-number/SL64ZBHICLRHVT7ISI77WQWKAW/graph.json","events_json":"https://pith.science/api/pith-number/SL64ZBHICLRHVT7ISI77WQWKAW/events.json","paper":"https://pith.science/paper/SL64ZBHI"},"agent_actions":{"view_html":"https://pith.science/pith/SL64ZBHICLRHVT7ISI77WQWKAW","download_json":"https://pith.science/pith/SL64ZBHICLRHVT7ISI77WQWKAW.json","view_paper":"https://pith.science/paper/SL64ZBHI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2602.23986&json=true","fetch_graph":"https://pith.science/api/pith-number/SL64ZBHICLRHVT7ISI77WQWKAW/graph.json","fetch_events":"https://pith.science/api/pith-number/SL64ZBHICLRHVT7ISI77WQWKAW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SL64ZBHICLRHVT7ISI77WQWKAW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SL64ZBHICLRHVT7ISI77WQWKAW/action/storage_attestation","attest_author":"https://pith.science/pith/SL64ZBHICLRHVT7ISI77WQWKAW/action/author_attestation","sign_citation":"https://pith.science/pith/SL64ZBHICLRHVT7ISI77WQWKAW/action/citation_signature","submit_replication":"https://pith.science/pith/SL64ZBHICLRHVT7ISI77WQWKAW/action/replication_record"}},"created_at":"2026-07-08T01:19:11.159348+00:00","updated_at":"2026-07-08T01:19:11.159348+00:00"}