{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:WNG42YKXLCGYVUMPALACAALJ6P","short_pith_number":"pith:WNG42YKX","schema_version":"1.0","canonical_sha256":"b34dcd6157588d8ad18f02c0200169f3fa81286a6f1664b557cbaab6bcfce597","source":{"kind":"arxiv","id":"hep-ph/0510237","version":4},"attestation_state":"computed","paper":{"title":"Light Cone Sum Rules for gamma* N -> Delta Transition Form Factors","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Lenz, A.V. Radyushkin, G. Peters, V.M. Braun","submitted_at":"2005-10-18T19:55:56Z","abstract_excerpt":"A theoretical framework is suggested for the calculation of gamma* N -> Delta transition form factors using the light-cone sum rule approach. Leading-order sum rules are derived and compared with the existing experimental data. We find that the transition form factors in a several GeV region are dominated by the ``soft'' contributions that can be thought of as overlap integrals of the valence components of the hadron wave functions. The ``minus'' components of the quark fields contribute significantly to the result, which can be reinterpreted as large contributions of the quark orbital angular"},"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/0510237","kind":"arxiv","version":4},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2005-10-18T19:55:56Z","cross_cats_sorted":[],"title_canon_sha256":"1992771218e381e84f68f70db6d58186e318e6b95d4fd3a2a9e088287fbc4b23","abstract_canon_sha256":"a113970eafa23f9589ebd7aeb78c11fbfe2164097609a7faa5341625fc5e4e8b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:36:19.176470Z","signature_b64":"AEH8n50x1E6vAsSVgd8BFx2y4ne74WN9IlYepVkcrPduTHW+68lqMKbv7skivqDPHhVWxAgeYGjnOmSMojurDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b34dcd6157588d8ad18f02c0200169f3fa81286a6f1664b557cbaab6bcfce597","last_reissued_at":"2026-05-18T02:36:19.175850Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:36:19.175850Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Light Cone Sum Rules for gamma* N -> Delta Transition Form Factors","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Lenz, A.V. Radyushkin, G. Peters, V.M. Braun","submitted_at":"2005-10-18T19:55:56Z","abstract_excerpt":"A theoretical framework is suggested for the calculation of gamma* N -> Delta transition form factors using the light-cone sum rule approach. Leading-order sum rules are derived and compared with the existing experimental data. We find that the transition form factors in a several GeV region are dominated by the ``soft'' contributions that can be thought of as overlap integrals of the valence components of the hadron wave functions. The ``minus'' components of the quark fields contribute significantly to the result, which can be reinterpreted as large contributions of the quark orbital angular"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0510237","kind":"arxiv","version":4},"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/0510237","created_at":"2026-05-18T02:36:19.175936+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0510237v4","created_at":"2026-05-18T02:36:19.175936+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0510237","created_at":"2026-05-18T02:36:19.175936+00:00"},{"alias_kind":"pith_short_12","alias_value":"WNG42YKXLCGY","created_at":"2026-05-18T12:25:53.939244+00:00"},{"alias_kind":"pith_short_16","alias_value":"WNG42YKXLCGYVUMP","created_at":"2026-05-18T12:25:53.939244+00:00"},{"alias_kind":"pith_short_8","alias_value":"WNG42YKX","created_at":"2026-05-18T12:25:53.939244+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/WNG42YKXLCGYVUMPALACAALJ6P","json":"https://pith.science/pith/WNG42YKXLCGYVUMPALACAALJ6P.json","graph_json":"https://pith.science/api/pith-number/WNG42YKXLCGYVUMPALACAALJ6P/graph.json","events_json":"https://pith.science/api/pith-number/WNG42YKXLCGYVUMPALACAALJ6P/events.json","paper":"https://pith.science/paper/WNG42YKX"},"agent_actions":{"view_html":"https://pith.science/pith/WNG42YKXLCGYVUMPALACAALJ6P","download_json":"https://pith.science/pith/WNG42YKXLCGYVUMPALACAALJ6P.json","view_paper":"https://pith.science/paper/WNG42YKX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0510237&json=true","fetch_graph":"https://pith.science/api/pith-number/WNG42YKXLCGYVUMPALACAALJ6P/graph.json","fetch_events":"https://pith.science/api/pith-number/WNG42YKXLCGYVUMPALACAALJ6P/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WNG42YKXLCGYVUMPALACAALJ6P/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WNG42YKXLCGYVUMPALACAALJ6P/action/storage_attestation","attest_author":"https://pith.science/pith/WNG42YKXLCGYVUMPALACAALJ6P/action/author_attestation","sign_citation":"https://pith.science/pith/WNG42YKXLCGYVUMPALACAALJ6P/action/citation_signature","submit_replication":"https://pith.science/pith/WNG42YKXLCGYVUMPALACAALJ6P/action/replication_record"}},"created_at":"2026-05-18T02:36:19.175936+00:00","updated_at":"2026-05-18T02:36:19.175936+00:00"}