{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1997:EO3GTSODWFXGKUSDQMSXPHLTZW","short_pith_number":"pith:EO3GTSOD","schema_version":"1.0","canonical_sha256":"23b669c9c3b16e6552438325779d73cda79204056e89112d16bb9ea8f659dd61","source":{"kind":"arxiv","id":"hep-ph/9702269","version":1},"attestation_state":"computed","paper":{"title":"Omega-Phi mixing at finite temperature","license":"","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"(2) University of Minnesota), Charles Gale (1), David Seibert (1), Joseph Kapusta (2) ((1) McGill University","submitted_at":"1997-02-05T21:13:48Z","abstract_excerpt":"We compute the mass shifts and mixing of the Omega and Phi mesons at finite temperature due to scattering from thermal pions. The Rho and b_1 mesons are important intermediate states. Up to a temperature of 140 MeV the Omega mass increases by 12 MeV and the Phi mass decreases by 0.6 MeV. The change in mixing angles is negligible."},"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":"hep-ph/9702269","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1997-02-05T21:13:48Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"eca182a4987b551586fc1673e8b64946967d6d0f1575c92832c428477ee8edd4","abstract_canon_sha256":"3ac97f3692669a6b11bbe99928865dd055d4cd015127918818ae3138fd0f5e65"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:37:05.324973Z","signature_b64":"G7PE1YcQPePpZSkp4sw8b7yPFIfss/IHyKPCAH0kKlg6Vmeo7RbVeIiiIkrjYz7FCOvf920WkkkCYz6xIMbZDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"23b669c9c3b16e6552438325779d73cda79204056e89112d16bb9ea8f659dd61","last_reissued_at":"2026-05-18T02:37:05.324311Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:37:05.324311Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Omega-Phi mixing at finite temperature","license":"","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"(2) University of Minnesota), Charles Gale (1), David Seibert (1), Joseph Kapusta (2) ((1) McGill University","submitted_at":"1997-02-05T21:13:48Z","abstract_excerpt":"We compute the mass shifts and mixing of the Omega and Phi mesons at finite temperature due to scattering from thermal pions. The Rho and b_1 mesons are important intermediate states. Up to a temperature of 140 MeV the Omega mass increases by 12 MeV and the Phi mass decreases by 0.6 MeV. The change in mixing angles is negligible."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9702269","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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":"hep-ph/9702269","created_at":"2026-05-18T02:37:05.324421+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9702269v1","created_at":"2026-05-18T02:37:05.324421+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9702269","created_at":"2026-05-18T02:37:05.324421+00:00"},{"alias_kind":"pith_short_12","alias_value":"EO3GTSODWFXG","created_at":"2026-05-18T12:25:48.327863+00:00"},{"alias_kind":"pith_short_16","alias_value":"EO3GTSODWFXGKUSD","created_at":"2026-05-18T12:25:48.327863+00:00"},{"alias_kind":"pith_short_8","alias_value":"EO3GTSOD","created_at":"2026-05-18T12:25:48.327863+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/EO3GTSODWFXGKUSDQMSXPHLTZW","json":"https://pith.science/pith/EO3GTSODWFXGKUSDQMSXPHLTZW.json","graph_json":"https://pith.science/api/pith-number/EO3GTSODWFXGKUSDQMSXPHLTZW/graph.json","events_json":"https://pith.science/api/pith-number/EO3GTSODWFXGKUSDQMSXPHLTZW/events.json","paper":"https://pith.science/paper/EO3GTSOD"},"agent_actions":{"view_html":"https://pith.science/pith/EO3GTSODWFXGKUSDQMSXPHLTZW","download_json":"https://pith.science/pith/EO3GTSODWFXGKUSDQMSXPHLTZW.json","view_paper":"https://pith.science/paper/EO3GTSOD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9702269&json=true","fetch_graph":"https://pith.science/api/pith-number/EO3GTSODWFXGKUSDQMSXPHLTZW/graph.json","fetch_events":"https://pith.science/api/pith-number/EO3GTSODWFXGKUSDQMSXPHLTZW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EO3GTSODWFXGKUSDQMSXPHLTZW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EO3GTSODWFXGKUSDQMSXPHLTZW/action/storage_attestation","attest_author":"https://pith.science/pith/EO3GTSODWFXGKUSDQMSXPHLTZW/action/author_attestation","sign_citation":"https://pith.science/pith/EO3GTSODWFXGKUSDQMSXPHLTZW/action/citation_signature","submit_replication":"https://pith.science/pith/EO3GTSODWFXGKUSDQMSXPHLTZW/action/replication_record"}},"created_at":"2026-05-18T02:37:05.324421+00:00","updated_at":"2026-05-18T02:37:05.324421+00:00"}