{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:G5PXNIRDYGCIB6QSGJKYDYZ5N6","short_pith_number":"pith:G5PXNIRD","schema_version":"1.0","canonical_sha256":"375f76a223c18480fa12325581e33d6f83aa39a09482d625e1c7ad998ebe49af","source":{"kind":"arxiv","id":"2311.13101","version":1},"attestation_state":"computed","paper":{"title":"Analysis of the data for $\\gamma p \\to f_1(1285) p$ photoproduction","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Ai-Chao Wang, Fei Huang, Neng-Chang Wei","submitted_at":"2023-11-22T02:03:45Z","abstract_excerpt":"The photoproduction of $f_1(1285)$ meson off proton is investigated within an effective Lagrangian approach. The $t$-channel $\\rho$- and $\\omega$-exchange diagrams, $u$-channel nucleon-exchange diagram, generalized contact term, and $s$-channel pole diagrams of nucleon and a minimal number of nucleon resonances are taken into account in constructing the reaction amplitudes to describe the experimental data. Three different models, i.e., the Feynman model, the Regge model, and the interpolated Regge model, are employed where the $t$-channel reaction amplitudes are constructed in Feynman type, R"},"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":"2311.13101","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-11-22T02:03:45Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"bea0f9b3be809e242ce698610258e5718e7b0eca87cd2f220f2c3802f57c348e","abstract_canon_sha256":"8281f23f243ad6d72a68d982d91c532a7c43303f459b6fe62d37e622bc8e50c0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:04:35.641627Z","signature_b64":"vLrRzELNUnrfZ178CZNQcXhJJoWbQ8+ihERAF89F1ozQ5L9ckcJMdF6Z2eASqO0o0qxslSvBE5HXAr2ouc51Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"375f76a223c18480fa12325581e33d6f83aa39a09482d625e1c7ad998ebe49af","last_reissued_at":"2026-07-05T08:04:35.641121Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:04:35.641121Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Analysis of the data for $\\gamma p \\to f_1(1285) p$ photoproduction","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Ai-Chao Wang, Fei Huang, Neng-Chang Wei","submitted_at":"2023-11-22T02:03:45Z","abstract_excerpt":"The photoproduction of $f_1(1285)$ meson off proton is investigated within an effective Lagrangian approach. The $t$-channel $\\rho$- and $\\omega$-exchange diagrams, $u$-channel nucleon-exchange diagram, generalized contact term, and $s$-channel pole diagrams of nucleon and a minimal number of nucleon resonances are taken into account in constructing the reaction amplitudes to describe the experimental data. Three different models, i.e., the Feynman model, the Regge model, and the interpolated Regge model, are employed where the $t$-channel reaction amplitudes are constructed in Feynman type, R"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2311.13101","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2311.13101/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":"2311.13101","created_at":"2026-07-05T08:04:35.641185+00:00"},{"alias_kind":"arxiv_version","alias_value":"2311.13101v1","created_at":"2026-07-05T08:04:35.641185+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2311.13101","created_at":"2026-07-05T08:04:35.641185+00:00"},{"alias_kind":"pith_short_12","alias_value":"G5PXNIRDYGCI","created_at":"2026-07-05T08:04:35.641185+00:00"},{"alias_kind":"pith_short_16","alias_value":"G5PXNIRDYGCIB6QS","created_at":"2026-07-05T08:04:35.641185+00:00"},{"alias_kind":"pith_short_8","alias_value":"G5PXNIRD","created_at":"2026-07-05T08:04:35.641185+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/G5PXNIRDYGCIB6QSGJKYDYZ5N6","json":"https://pith.science/pith/G5PXNIRDYGCIB6QSGJKYDYZ5N6.json","graph_json":"https://pith.science/api/pith-number/G5PXNIRDYGCIB6QSGJKYDYZ5N6/graph.json","events_json":"https://pith.science/api/pith-number/G5PXNIRDYGCIB6QSGJKYDYZ5N6/events.json","paper":"https://pith.science/paper/G5PXNIRD"},"agent_actions":{"view_html":"https://pith.science/pith/G5PXNIRDYGCIB6QSGJKYDYZ5N6","download_json":"https://pith.science/pith/G5PXNIRDYGCIB6QSGJKYDYZ5N6.json","view_paper":"https://pith.science/paper/G5PXNIRD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2311.13101&json=true","fetch_graph":"https://pith.science/api/pith-number/G5PXNIRDYGCIB6QSGJKYDYZ5N6/graph.json","fetch_events":"https://pith.science/api/pith-number/G5PXNIRDYGCIB6QSGJKYDYZ5N6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/G5PXNIRDYGCIB6QSGJKYDYZ5N6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/G5PXNIRDYGCIB6QSGJKYDYZ5N6/action/storage_attestation","attest_author":"https://pith.science/pith/G5PXNIRDYGCIB6QSGJKYDYZ5N6/action/author_attestation","sign_citation":"https://pith.science/pith/G5PXNIRDYGCIB6QSGJKYDYZ5N6/action/citation_signature","submit_replication":"https://pith.science/pith/G5PXNIRDYGCIB6QSGJKYDYZ5N6/action/replication_record"}},"created_at":"2026-07-05T08:04:35.641185+00:00","updated_at":"2026-07-05T08:04:35.641185+00:00"}