{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1997:NK3G5J4A4F3TP7NDAQUMXCGGWC","short_pith_number":"pith:NK3G5J4A","schema_version":"1.0","canonical_sha256":"6ab66ea780e17737fda30428cb88c6b08ee7cdc636956e7c62256cca0c76455a","source":{"kind":"arxiv","id":"hep-ph/9711284","version":3},"attestation_state":"computed","paper":{"title":"Large corrections to asymptotic $F_{\\eta_c \\gamma}$ and $F_{\\eta_b \\gamma}$ in the light-cone perturbative QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Fu-Guang Cao, Tao Huang","submitted_at":"1997-11-11T06:39:04Z","abstract_excerpt":"The large-$Q^2$ behavior of $\\eta_c$-$\\gamma$ and $\\eta_b$-$\\gamma$ transition form factors, $F_{\\eta_c\\gamma}(Q^2)$ and $F_{\\eta_b\\gamma}(Q^2)$ are analyzed in the framework of light-cone perturbative QCD with the heavy quark ($c$ and $b$) mass effect, the parton's transverse momentum dependence and the higher helicity components in the light-cone wave function are respected. It is pointed out that the quark mass effect brings significant modifications to the asymptotic predictions of the transition form factors in a rather broad energy region, and this modification is much severer for $F_{\\e"},"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/9711284","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1997-11-11T06:39:04Z","cross_cats_sorted":[],"title_canon_sha256":"28f50415d6f72710a0d1d3f2e7d09ef4db036e55c9c23ac0643cae8a5a07ee60","abstract_canon_sha256":"78cd940c34104aa015e7b808808b7c3638367d7f043e52882281fe73ad83d0d6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:30:37.245839Z","signature_b64":"vCq/2MgnXvw4/EElhHCRBJ5DbjsUc5t/8UIY2uIp+hikWHoztqd+QKydnikrwafNxMMT8C5p6Nk4L+ua7cLzDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6ab66ea780e17737fda30428cb88c6b08ee7cdc636956e7c62256cca0c76455a","last_reissued_at":"2026-05-18T04:30:37.245128Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:30:37.245128Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Large corrections to asymptotic $F_{\\eta_c \\gamma}$ and $F_{\\eta_b \\gamma}$ in the light-cone perturbative QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Fu-Guang Cao, Tao Huang","submitted_at":"1997-11-11T06:39:04Z","abstract_excerpt":"The large-$Q^2$ behavior of $\\eta_c$-$\\gamma$ and $\\eta_b$-$\\gamma$ transition form factors, $F_{\\eta_c\\gamma}(Q^2)$ and $F_{\\eta_b\\gamma}(Q^2)$ are analyzed in the framework of light-cone perturbative QCD with the heavy quark ($c$ and $b$) mass effect, the parton's transverse momentum dependence and the higher helicity components in the light-cone wave function are respected. It is pointed out that the quark mass effect brings significant modifications to the asymptotic predictions of the transition form factors in a rather broad energy region, and this modification is much severer for $F_{\\e"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9711284","kind":"arxiv","version":3},"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/9711284","created_at":"2026-05-18T04:30:37.245251+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9711284v3","created_at":"2026-05-18T04:30:37.245251+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9711284","created_at":"2026-05-18T04:30:37.245251+00:00"},{"alias_kind":"pith_short_12","alias_value":"NK3G5J4A4F3T","created_at":"2026-05-18T12:25:48.327863+00:00"},{"alias_kind":"pith_short_16","alias_value":"NK3G5J4A4F3TP7ND","created_at":"2026-05-18T12:25:48.327863+00:00"},{"alias_kind":"pith_short_8","alias_value":"NK3G5J4A","created_at":"2026-05-18T12:25:48.327863+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2511.12996","citing_title":"Radiative Decays of Vector Mesons with Light-Cone Sum Rules","ref_index":72,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NK3G5J4A4F3TP7NDAQUMXCGGWC","json":"https://pith.science/pith/NK3G5J4A4F3TP7NDAQUMXCGGWC.json","graph_json":"https://pith.science/api/pith-number/NK3G5J4A4F3TP7NDAQUMXCGGWC/graph.json","events_json":"https://pith.science/api/pith-number/NK3G5J4A4F3TP7NDAQUMXCGGWC/events.json","paper":"https://pith.science/paper/NK3G5J4A"},"agent_actions":{"view_html":"https://pith.science/pith/NK3G5J4A4F3TP7NDAQUMXCGGWC","download_json":"https://pith.science/pith/NK3G5J4A4F3TP7NDAQUMXCGGWC.json","view_paper":"https://pith.science/paper/NK3G5J4A","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9711284&json=true","fetch_graph":"https://pith.science/api/pith-number/NK3G5J4A4F3TP7NDAQUMXCGGWC/graph.json","fetch_events":"https://pith.science/api/pith-number/NK3G5J4A4F3TP7NDAQUMXCGGWC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NK3G5J4A4F3TP7NDAQUMXCGGWC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NK3G5J4A4F3TP7NDAQUMXCGGWC/action/storage_attestation","attest_author":"https://pith.science/pith/NK3G5J4A4F3TP7NDAQUMXCGGWC/action/author_attestation","sign_citation":"https://pith.science/pith/NK3G5J4A4F3TP7NDAQUMXCGGWC/action/citation_signature","submit_replication":"https://pith.science/pith/NK3G5J4A4F3TP7NDAQUMXCGGWC/action/replication_record"}},"created_at":"2026-05-18T04:30:37.245251+00:00","updated_at":"2026-05-18T04:30:37.245251+00:00"}