{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:4TT4KE5GZQ3LAER6QIGJ6BYZR2","short_pith_number":"pith:4TT4KE5G","schema_version":"1.0","canonical_sha256":"e4e7c513a6cc36b0123e820c9f07198eb680e79828c745bcd05866911881a1d3","source":{"kind":"arxiv","id":"1711.07156","version":2},"attestation_state":"computed","paper":{"title":"Subleading hadronic vacuum polarization contributions to muon $g-2$: $\\mu^+\\mu^- \\rightarrow \\gamma^* \\rightarrow \\pi^0 \\gamma^*$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Deog Ki Hong, Du Hwan Kim, Jong-Wan Lee","submitted_at":"2017-11-20T05:46:42Z","abstract_excerpt":"We consider the subleading contributions of the hadronic vacuum polarization, involving the $\\pi^0\\gamma^*\\gamma^*$ transition form factor, to the muon anomalous magnetic moment $g-2$. Various models for the form factor, based on hadronic ansatzes and holographic principles, are considered: They are the Wess-Zumino-Witten, vector meson dominance, lowest meson dominance (one and two vector resonances) models, and AdS/QCD. The model parameters are determined by fitting the experimental data for the $e^+ e^- \\rightarrow \\pi^0 \\gamma$ total cross section. We report numerical results of the correct"},"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":"1711.07156","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-11-20T05:46:42Z","cross_cats_sorted":[],"title_canon_sha256":"9a92fe793c4ba45782bbfed851b4dda453da7d255e298a82baf44ca08b3a2765","abstract_canon_sha256":"f8576ec1f6b0cdda9a1c233d8e8b58709e419ea304f25095b35a0f8adf4ea1e2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:23:29.328976Z","signature_b64":"iadLnnYxlixsD6Ycss+BtfB7cRgN19W/srjUkxbyEetQDkdqtcYD4YfKHLUYz6OGrPh3VM5kCmBQq8JJGLXDCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e4e7c513a6cc36b0123e820c9f07198eb680e79828c745bcd05866911881a1d3","last_reissued_at":"2026-05-18T00:23:29.328450Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:23:29.328450Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Subleading hadronic vacuum polarization contributions to muon $g-2$: $\\mu^+\\mu^- \\rightarrow \\gamma^* \\rightarrow \\pi^0 \\gamma^*$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Deog Ki Hong, Du Hwan Kim, Jong-Wan Lee","submitted_at":"2017-11-20T05:46:42Z","abstract_excerpt":"We consider the subleading contributions of the hadronic vacuum polarization, involving the $\\pi^0\\gamma^*\\gamma^*$ transition form factor, to the muon anomalous magnetic moment $g-2$. Various models for the form factor, based on hadronic ansatzes and holographic principles, are considered: They are the Wess-Zumino-Witten, vector meson dominance, lowest meson dominance (one and two vector resonances) models, and AdS/QCD. The model parameters are determined by fitting the experimental data for the $e^+ e^- \\rightarrow \\pi^0 \\gamma$ total cross section. We report numerical results of the correct"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.07156","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":""},"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":"1711.07156","created_at":"2026-05-18T00:23:29.328530+00:00"},{"alias_kind":"arxiv_version","alias_value":"1711.07156v2","created_at":"2026-05-18T00:23:29.328530+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.07156","created_at":"2026-05-18T00:23:29.328530+00:00"},{"alias_kind":"pith_short_12","alias_value":"4TT4KE5GZQ3L","created_at":"2026-05-18T12:31:00.734936+00:00"},{"alias_kind":"pith_short_16","alias_value":"4TT4KE5GZQ3LAER6","created_at":"2026-05-18T12:31:00.734936+00:00"},{"alias_kind":"pith_short_8","alias_value":"4TT4KE5G","created_at":"2026-05-18T12:31:00.734936+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/4TT4KE5GZQ3LAER6QIGJ6BYZR2","json":"https://pith.science/pith/4TT4KE5GZQ3LAER6QIGJ6BYZR2.json","graph_json":"https://pith.science/api/pith-number/4TT4KE5GZQ3LAER6QIGJ6BYZR2/graph.json","events_json":"https://pith.science/api/pith-number/4TT4KE5GZQ3LAER6QIGJ6BYZR2/events.json","paper":"https://pith.science/paper/4TT4KE5G"},"agent_actions":{"view_html":"https://pith.science/pith/4TT4KE5GZQ3LAER6QIGJ6BYZR2","download_json":"https://pith.science/pith/4TT4KE5GZQ3LAER6QIGJ6BYZR2.json","view_paper":"https://pith.science/paper/4TT4KE5G","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1711.07156&json=true","fetch_graph":"https://pith.science/api/pith-number/4TT4KE5GZQ3LAER6QIGJ6BYZR2/graph.json","fetch_events":"https://pith.science/api/pith-number/4TT4KE5GZQ3LAER6QIGJ6BYZR2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4TT4KE5GZQ3LAER6QIGJ6BYZR2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4TT4KE5GZQ3LAER6QIGJ6BYZR2/action/storage_attestation","attest_author":"https://pith.science/pith/4TT4KE5GZQ3LAER6QIGJ6BYZR2/action/author_attestation","sign_citation":"https://pith.science/pith/4TT4KE5GZQ3LAER6QIGJ6BYZR2/action/citation_signature","submit_replication":"https://pith.science/pith/4TT4KE5GZQ3LAER6QIGJ6BYZR2/action/replication_record"}},"created_at":"2026-05-18T00:23:29.328530+00:00","updated_at":"2026-05-18T00:23:29.328530+00:00"}