{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:R5M7KEJ2RLZ4WBBOKKCQJHUIOO","short_pith_number":"pith:R5M7KEJ2","schema_version":"1.0","canonical_sha256":"8f59f5113a8af3cb042e5285049e8873851201167311830d240386e8869d2999","source":{"kind":"arxiv","id":"1912.01596","version":5},"attestation_state":"computed","paper":{"title":"Axial vector transition form factors in holographic QCD and their contribution to the anomalous magnetic moment of the muon","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Anton Rebhan, Josef Leutgeb","submitted_at":"2019-12-03T18:48:59Z","abstract_excerpt":"We evaluate axial vector transition form factors in holographic QCD models that have been shown to reproduce well recent experimental and theoretical results for the pion transition form factor. Comparing with L3 data on $f_1\\to\\gamma\\gamma^*$ we find remarkable agreement regarding the shape of single-virtual form factors. In the double-virtual case, the holographic results differ strongly from a simple dipole form, and this has an important impact on the corresponding estimate of the axial vector contribution to the anomalous magnetic moment of the muon $a_\\mu$ through hadronic light-by-light"},"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":"1912.01596","kind":"arxiv","version":5},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-12-03T18:48:59Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"9ab4fa85c0bcd692968be3aa3a45c5c477b6688ed9626f836642a49087df7b1b","abstract_canon_sha256":"806f0ab27123d0b85080c555f363bacc53054957c497decbf2fbdc5609ca5d98"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:22:29.259507Z","signature_b64":"dMv17BGOHbSGTZyuoJbOfFGDms1xzcsKi+rehu6y57GFC88FDR301sNoROAxQZznodUJalX7rt2+4Fr4ZFJCDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8f59f5113a8af3cb042e5285049e8873851201167311830d240386e8869d2999","last_reissued_at":"2026-07-05T08:22:29.259020Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:22:29.259020Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Axial vector transition form factors in holographic QCD and their contribution to the anomalous magnetic moment of the muon","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Anton Rebhan, Josef Leutgeb","submitted_at":"2019-12-03T18:48:59Z","abstract_excerpt":"We evaluate axial vector transition form factors in holographic QCD models that have been shown to reproduce well recent experimental and theoretical results for the pion transition form factor. Comparing with L3 data on $f_1\\to\\gamma\\gamma^*$ we find remarkable agreement regarding the shape of single-virtual form factors. In the double-virtual case, the holographic results differ strongly from a simple dipole form, and this has an important impact on the corresponding estimate of the axial vector contribution to the anomalous magnetic moment of the muon $a_\\mu$ through hadronic light-by-light"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1912.01596","kind":"arxiv","version":5},"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/1912.01596/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":"1912.01596","created_at":"2026-07-05T08:22:29.259082+00:00"},{"alias_kind":"arxiv_version","alias_value":"1912.01596v5","created_at":"2026-07-05T08:22:29.259082+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1912.01596","created_at":"2026-07-05T08:22:29.259082+00:00"},{"alias_kind":"pith_short_12","alias_value":"R5M7KEJ2RLZ4","created_at":"2026-07-05T08:22:29.259082+00:00"},{"alias_kind":"pith_short_16","alias_value":"R5M7KEJ2RLZ4WBBO","created_at":"2026-07-05T08:22:29.259082+00:00"},{"alias_kind":"pith_short_8","alias_value":"R5M7KEJ2","created_at":"2026-07-05T08:22:29.259082+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":6,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2607.00564","citing_title":"Isospin-breaking effects in inclusive hadronic $\\tau$ data for the muon $(g-2)$ from first principles","ref_index":11,"is_internal_anchor":false},{"citing_arxiv_id":"2510.13966","citing_title":"Light new physics and the $\\tau$ lepton dipole moments: prospects at Belle II","ref_index":58,"is_internal_anchor":false},{"citing_arxiv_id":"2511.03786","citing_title":"Light new physics and the $\\tau$ lepton dipole moments","ref_index":64,"is_internal_anchor":false},{"citing_arxiv_id":"2505.21476","citing_title":"The anomalous magnetic moment of the muon in the Standard Model: an update","ref_index":40,"is_internal_anchor":false},{"citing_arxiv_id":"2605.03209","citing_title":"Elastic Form Factors of Axial-Vector Mesons: A Contact Interaction Exploration","ref_index":18,"is_internal_anchor":false},{"citing_arxiv_id":"2604.25004","citing_title":"Muon $g$$-$2: correlation-induced uncertainties in precision data combinations","ref_index":70,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/R5M7KEJ2RLZ4WBBOKKCQJHUIOO","json":"https://pith.science/pith/R5M7KEJ2RLZ4WBBOKKCQJHUIOO.json","graph_json":"https://pith.science/api/pith-number/R5M7KEJ2RLZ4WBBOKKCQJHUIOO/graph.json","events_json":"https://pith.science/api/pith-number/R5M7KEJ2RLZ4WBBOKKCQJHUIOO/events.json","paper":"https://pith.science/paper/R5M7KEJ2"},"agent_actions":{"view_html":"https://pith.science/pith/R5M7KEJ2RLZ4WBBOKKCQJHUIOO","download_json":"https://pith.science/pith/R5M7KEJ2RLZ4WBBOKKCQJHUIOO.json","view_paper":"https://pith.science/paper/R5M7KEJ2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1912.01596&json=true","fetch_graph":"https://pith.science/api/pith-number/R5M7KEJ2RLZ4WBBOKKCQJHUIOO/graph.json","fetch_events":"https://pith.science/api/pith-number/R5M7KEJ2RLZ4WBBOKKCQJHUIOO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/R5M7KEJ2RLZ4WBBOKKCQJHUIOO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/R5M7KEJ2RLZ4WBBOKKCQJHUIOO/action/storage_attestation","attest_author":"https://pith.science/pith/R5M7KEJ2RLZ4WBBOKKCQJHUIOO/action/author_attestation","sign_citation":"https://pith.science/pith/R5M7KEJ2RLZ4WBBOKKCQJHUIOO/action/citation_signature","submit_replication":"https://pith.science/pith/R5M7KEJ2RLZ4WBBOKKCQJHUIOO/action/replication_record"}},"created_at":"2026-07-05T08:22:29.259082+00:00","updated_at":"2026-07-05T08:22:29.259082+00:00"}