{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:6EY2E5LRKUPY4HAUPFOAMLTF6L","short_pith_number":"pith:6EY2E5LR","schema_version":"1.0","canonical_sha256":"f131a27571551f8e1c14795c062e65f2cce78fa3c5fcb8490ff2328488adfb2b","source":{"kind":"arxiv","id":"2405.15823","version":2},"attestation_state":"computed","paper":{"title":"Minimal Models and Transport Properties of Unconventional $p$-Wave Magnets","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Arne Brataas, Bj{\\o}rnulf Brekke, Hans Gl{\\o}ckner Giil, Jacob Linder, Pavlo Sukhachov","submitted_at":"2024-05-23T18:00:00Z","abstract_excerpt":"New unconventional compensated magnets with a $p$-wave spin polarization protected by a composite time-reversal translation symmetry have been proposed in the wake of altermagnets. To facilitate the experimental discovery and applications of these unconventional magnets, we construct an effective analytical model. The effective model is based on a minimal tight-binding model for unconventional $p$-wave magnets that clarifies the relation to other magnets with $p$-wave spin-polarized bands. One of the most prominent advantages of our analytical model is the possibility to employ various analyti"},"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":"2405.15823","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2024-05-23T18:00:00Z","cross_cats_sorted":[],"title_canon_sha256":"4e64b00e53a2001a050a222ed0a4cb0c769cea6add2573e37d58fde3dc9446d5","abstract_canon_sha256":"12e31d11a955980e33769402e12a7909e3b17c706254a3b5fcabb1f0d0443ac9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:47:30.352676Z","signature_b64":"e6hUpzqAssfX1r3bGuFC3TN6zsdNpA9rUK/cLFNLFk74DtUaR4z+BA1TmM6e8INNFGHtE+nhwr0BOVGUu3huBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f131a27571551f8e1c14795c062e65f2cce78fa3c5fcb8490ff2328488adfb2b","last_reissued_at":"2026-07-05T09:47:30.352166Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:47:30.352166Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Minimal Models and Transport Properties of Unconventional $p$-Wave Magnets","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Arne Brataas, Bj{\\o}rnulf Brekke, Hans Gl{\\o}ckner Giil, Jacob Linder, Pavlo Sukhachov","submitted_at":"2024-05-23T18:00:00Z","abstract_excerpt":"New unconventional compensated magnets with a $p$-wave spin polarization protected by a composite time-reversal translation symmetry have been proposed in the wake of altermagnets. To facilitate the experimental discovery and applications of these unconventional magnets, we construct an effective analytical model. The effective model is based on a minimal tight-binding model for unconventional $p$-wave magnets that clarifies the relation to other magnets with $p$-wave spin-polarized bands. One of the most prominent advantages of our analytical model is the possibility to employ various analyti"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2405.15823","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/2405.15823/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":"2405.15823","created_at":"2026-07-05T09:47:30.352224+00:00"},{"alias_kind":"arxiv_version","alias_value":"2405.15823v2","created_at":"2026-07-05T09:47:30.352224+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2405.15823","created_at":"2026-07-05T09:47:30.352224+00:00"},{"alias_kind":"pith_short_12","alias_value":"6EY2E5LRKUPY","created_at":"2026-07-05T09:47:30.352224+00:00"},{"alias_kind":"pith_short_16","alias_value":"6EY2E5LRKUPY4HAU","created_at":"2026-07-05T09:47:30.352224+00:00"},{"alias_kind":"pith_short_8","alias_value":"6EY2E5LR","created_at":"2026-07-05T09:47:30.352224+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.18695","citing_title":"$P$-wave Orbital Magnetism","ref_index":14,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6EY2E5LRKUPY4HAUPFOAMLTF6L","json":"https://pith.science/pith/6EY2E5LRKUPY4HAUPFOAMLTF6L.json","graph_json":"https://pith.science/api/pith-number/6EY2E5LRKUPY4HAUPFOAMLTF6L/graph.json","events_json":"https://pith.science/api/pith-number/6EY2E5LRKUPY4HAUPFOAMLTF6L/events.json","paper":"https://pith.science/paper/6EY2E5LR"},"agent_actions":{"view_html":"https://pith.science/pith/6EY2E5LRKUPY4HAUPFOAMLTF6L","download_json":"https://pith.science/pith/6EY2E5LRKUPY4HAUPFOAMLTF6L.json","view_paper":"https://pith.science/paper/6EY2E5LR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2405.15823&json=true","fetch_graph":"https://pith.science/api/pith-number/6EY2E5LRKUPY4HAUPFOAMLTF6L/graph.json","fetch_events":"https://pith.science/api/pith-number/6EY2E5LRKUPY4HAUPFOAMLTF6L/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6EY2E5LRKUPY4HAUPFOAMLTF6L/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6EY2E5LRKUPY4HAUPFOAMLTF6L/action/storage_attestation","attest_author":"https://pith.science/pith/6EY2E5LRKUPY4HAUPFOAMLTF6L/action/author_attestation","sign_citation":"https://pith.science/pith/6EY2E5LRKUPY4HAUPFOAMLTF6L/action/citation_signature","submit_replication":"https://pith.science/pith/6EY2E5LRKUPY4HAUPFOAMLTF6L/action/replication_record"}},"created_at":"2026-07-05T09:47:30.352224+00:00","updated_at":"2026-07-05T09:47:30.352224+00:00"}