{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:XEJ7I6ADCWL44WJQCPMT7TAPVQ","short_pith_number":"pith:XEJ7I6AD","schema_version":"1.0","canonical_sha256":"b913f478031597ce593013d93fcc0fac223bcd545d5fb2e7e8f3bdb775ae5631","source":{"kind":"arxiv","id":"1312.1226","version":1},"attestation_state":"computed","paper":{"title":"Axial anomaly and vector meson dominance model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Armen Oganesian, Oleg Teryaev, Yaroslav Klopot","submitted_at":"2013-12-04T16:06:09Z","abstract_excerpt":"The dispersive representation of axial anomaly leads to the anomaly sum rules (ASRs), exact nonperturbative relations in QCD. The analytical continuation of the ASRs to the time-like region is performed. The transition form factors of $\\pi^0$, $\\eta$ and $\\eta'$ mesons in this region are calculated. A good agreement with the available experimental data is found. Based on the ASRs, we have provided the foundations for the vector meson dominance model in these processes."},"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":"1312.1226","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-12-04T16:06:09Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"6ccd38bda009d180d6fc536ae98109ff4b2ac602fd49fdec146a6074ffc3e969","abstract_canon_sha256":"19a763a3c90b9ba093369b7d2c5edc7b8a4bc911b4dd6c8654eeebda9b034390"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:45:58.683698Z","signature_b64":"4oJ3G7s5zt3EyOyMtmpuuBRVIQhHvn9xIFeQS/NTF2PQ0zeb2/MkBljP+XkYxhz+poN/XPuRkxYdT5hxl9t2Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b913f478031597ce593013d93fcc0fac223bcd545d5fb2e7e8f3bdb775ae5631","last_reissued_at":"2026-05-18T01:45:58.683199Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:45:58.683199Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Axial anomaly and vector meson dominance model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Armen Oganesian, Oleg Teryaev, Yaroslav Klopot","submitted_at":"2013-12-04T16:06:09Z","abstract_excerpt":"The dispersive representation of axial anomaly leads to the anomaly sum rules (ASRs), exact nonperturbative relations in QCD. The analytical continuation of the ASRs to the time-like region is performed. The transition form factors of $\\pi^0$, $\\eta$ and $\\eta'$ mesons in this region are calculated. A good agreement with the available experimental data is found. Based on the ASRs, we have provided the foundations for the vector meson dominance model in these processes."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.1226","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":"1312.1226","created_at":"2026-05-18T01:45:58.683268+00:00"},{"alias_kind":"arxiv_version","alias_value":"1312.1226v1","created_at":"2026-05-18T01:45:58.683268+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.1226","created_at":"2026-05-18T01:45:58.683268+00:00"},{"alias_kind":"pith_short_12","alias_value":"XEJ7I6ADCWL4","created_at":"2026-05-18T12:28:06.772260+00:00"},{"alias_kind":"pith_short_16","alias_value":"XEJ7I6ADCWL44WJQ","created_at":"2026-05-18T12:28:06.772260+00:00"},{"alias_kind":"pith_short_8","alias_value":"XEJ7I6AD","created_at":"2026-05-18T12:28:06.772260+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/XEJ7I6ADCWL44WJQCPMT7TAPVQ","json":"https://pith.science/pith/XEJ7I6ADCWL44WJQCPMT7TAPVQ.json","graph_json":"https://pith.science/api/pith-number/XEJ7I6ADCWL44WJQCPMT7TAPVQ/graph.json","events_json":"https://pith.science/api/pith-number/XEJ7I6ADCWL44WJQCPMT7TAPVQ/events.json","paper":"https://pith.science/paper/XEJ7I6AD"},"agent_actions":{"view_html":"https://pith.science/pith/XEJ7I6ADCWL44WJQCPMT7TAPVQ","download_json":"https://pith.science/pith/XEJ7I6ADCWL44WJQCPMT7TAPVQ.json","view_paper":"https://pith.science/paper/XEJ7I6AD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1312.1226&json=true","fetch_graph":"https://pith.science/api/pith-number/XEJ7I6ADCWL44WJQCPMT7TAPVQ/graph.json","fetch_events":"https://pith.science/api/pith-number/XEJ7I6ADCWL44WJQCPMT7TAPVQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XEJ7I6ADCWL44WJQCPMT7TAPVQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XEJ7I6ADCWL44WJQCPMT7TAPVQ/action/storage_attestation","attest_author":"https://pith.science/pith/XEJ7I6ADCWL44WJQCPMT7TAPVQ/action/author_attestation","sign_citation":"https://pith.science/pith/XEJ7I6ADCWL44WJQCPMT7TAPVQ/action/citation_signature","submit_replication":"https://pith.science/pith/XEJ7I6ADCWL44WJQCPMT7TAPVQ/action/replication_record"}},"created_at":"2026-05-18T01:45:58.683268+00:00","updated_at":"2026-05-18T01:45:58.683268+00:00"}