{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:FDU6KJFBBM66W4WQFKGZZOIVKA","short_pith_number":"pith:FDU6KJFB","schema_version":"1.0","canonical_sha256":"28e9e524a10b3deb72d02a8d9cb9155010d4b33f2dd6c6ea51ddef0deb870210","source":{"kind":"arxiv","id":"hep-ph/9910273","version":1},"attestation_state":"computed","paper":{"title":"Hadron Electric Dipole Moments from CP-Odd Operators of Dimension Five Via QCD Sum Rules: The Vector Meson","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Adam Ritz, Maxim Pospelov","submitted_at":"1999-10-07T17:33:27Z","abstract_excerpt":"We present a complete analysis of the electric dipole moment (EDM) of the \\rho-meson induced by CP violating operators of dimension 4 and 5 within the QCD sum rules approach. The set of CP-odd operators includes the theta term and the electric and chromoelectric dipole moments of the three light quarks. We find that the \\rho-meson EDM induced purely by the EDMs of quarks is smaller, but still in reasonable agreement, with the predictions of a naive constituent quark model. However, the chromoelectric dipole moments, including that of the strange quark, give comparable and sometimes larger cont"},"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/9910273","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1999-10-07T17:33:27Z","cross_cats_sorted":[],"title_canon_sha256":"5dd78f84ea2465fb5c4bb80b9f097265e2bce301fc3df9c34820b5208db95ce0","abstract_canon_sha256":"3d980a57bd5b91f97961c535a19bacfcae72c1ba8048cd643456bd2f773f74b3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:14:30.899923Z","signature_b64":"jDVWKHFRrtXrJ/bLXrjEMWWFcNx1pG1Waxu2vqcIQD4EirBNaBcss4Urk6QaEhRyAd2ZIYYYrUhEdSsce9SEBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"28e9e524a10b3deb72d02a8d9cb9155010d4b33f2dd6c6ea51ddef0deb870210","last_reissued_at":"2026-07-04T16:14:30.899539Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:14:30.899539Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hadron Electric Dipole Moments from CP-Odd Operators of Dimension Five Via QCD Sum Rules: The Vector Meson","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Adam Ritz, Maxim Pospelov","submitted_at":"1999-10-07T17:33:27Z","abstract_excerpt":"We present a complete analysis of the electric dipole moment (EDM) of the \\rho-meson induced by CP violating operators of dimension 4 and 5 within the QCD sum rules approach. The set of CP-odd operators includes the theta term and the electric and chromoelectric dipole moments of the three light quarks. We find that the \\rho-meson EDM induced purely by the EDMs of quarks is smaller, but still in reasonable agreement, with the predictions of a naive constituent quark model. However, the chromoelectric dipole moments, including that of the strange quark, give comparable and sometimes larger cont"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9910273","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/9910273/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":"hep-ph/9910273","created_at":"2026-07-04T16:14:30.899603+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9910273v1","created_at":"2026-07-04T16:14:30.899603+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9910273","created_at":"2026-07-04T16:14:30.899603+00:00"},{"alias_kind":"pith_short_12","alias_value":"FDU6KJFBBM66","created_at":"2026-07-04T16:14:30.899603+00:00"},{"alias_kind":"pith_short_16","alias_value":"FDU6KJFBBM66W4WQ","created_at":"2026-07-04T16:14:30.899603+00:00"},{"alias_kind":"pith_short_8","alias_value":"FDU6KJFB","created_at":"2026-07-04T16:14:30.899603+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2604.25516","citing_title":"The EDM inverse problem: Identifying the sources of CP violation and PQ breaking with electric dipole moments","ref_index":33,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FDU6KJFBBM66W4WQFKGZZOIVKA","json":"https://pith.science/pith/FDU6KJFBBM66W4WQFKGZZOIVKA.json","graph_json":"https://pith.science/api/pith-number/FDU6KJFBBM66W4WQFKGZZOIVKA/graph.json","events_json":"https://pith.science/api/pith-number/FDU6KJFBBM66W4WQFKGZZOIVKA/events.json","paper":"https://pith.science/paper/FDU6KJFB"},"agent_actions":{"view_html":"https://pith.science/pith/FDU6KJFBBM66W4WQFKGZZOIVKA","download_json":"https://pith.science/pith/FDU6KJFBBM66W4WQFKGZZOIVKA.json","view_paper":"https://pith.science/paper/FDU6KJFB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9910273&json=true","fetch_graph":"https://pith.science/api/pith-number/FDU6KJFBBM66W4WQFKGZZOIVKA/graph.json","fetch_events":"https://pith.science/api/pith-number/FDU6KJFBBM66W4WQFKGZZOIVKA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FDU6KJFBBM66W4WQFKGZZOIVKA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FDU6KJFBBM66W4WQFKGZZOIVKA/action/storage_attestation","attest_author":"https://pith.science/pith/FDU6KJFBBM66W4WQFKGZZOIVKA/action/author_attestation","sign_citation":"https://pith.science/pith/FDU6KJFBBM66W4WQFKGZZOIVKA/action/citation_signature","submit_replication":"https://pith.science/pith/FDU6KJFBBM66W4WQFKGZZOIVKA/action/replication_record"}},"created_at":"2026-07-04T16:14:30.899603+00:00","updated_at":"2026-07-04T16:14:30.899603+00:00"}