{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:M4GXVVNUX4PG6UJGEMYYJBLRRG","short_pith_number":"pith:M4GXVVNU","schema_version":"1.0","canonical_sha256":"670d7ad5b4bf1e6f5126233184857189b55934180c954f4e8cbb857af8aa2f19","source":{"kind":"arxiv","id":"2403.19384","version":2},"attestation_state":"computed","paper":{"title":"Impact of JLab data on the determination of GPDs at zero skewness and new insights from transition form factors $ N\\rightarrow \\Delta $","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Fatemeh Irani, Hadi Hashamipour, K. Azizi, Muhammad Goharipour, The MMGPDs Collaboration","submitted_at":"2024-03-28T12:45:43Z","abstract_excerpt":"It is well established now that the generalized parton distributions (GPDs) at zero skewness are playing important roles in some physical process such as elastic electron-nucleon scattering, elastic (anti)neutrino-nucleon scattering, and wide-angle Compton scattering (WACS) via various types of form factors (FFs). In this study, we are going to utilize the recent JLab measurements of the elastic electron-nucleon scattering reduced cross-section, namely GMp12, as a touchstone to unravel the tension observed between the measurements of the WACS cross-section and the data of the proton magnetic F"},"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":"2403.19384","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-03-28T12:45:43Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"3da23ddebf2d69e659b3b9fce476155ef56a7ea2b87989147e6d9848ccaf46e3","abstract_canon_sha256":"030a327bac98c9ab34438f58ab8053182bfab2846d84bfaef1886a339c1a22f4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:14:04.959572Z","signature_b64":"OCHwGOz3HIR4w9DYLG29ibJWWOHMqMIWrSLcRuErFWvQHW1jg7ck8Qv0zon+4gjcWlzXjh3hdZb4W/ArZi+wDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"670d7ad5b4bf1e6f5126233184857189b55934180c954f4e8cbb857af8aa2f19","last_reissued_at":"2026-07-05T08:14:04.959093Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:14:04.959093Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Impact of JLab data on the determination of GPDs at zero skewness and new insights from transition form factors $ N\\rightarrow \\Delta $","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Fatemeh Irani, Hadi Hashamipour, K. Azizi, Muhammad Goharipour, The MMGPDs Collaboration","submitted_at":"2024-03-28T12:45:43Z","abstract_excerpt":"It is well established now that the generalized parton distributions (GPDs) at zero skewness are playing important roles in some physical process such as elastic electron-nucleon scattering, elastic (anti)neutrino-nucleon scattering, and wide-angle Compton scattering (WACS) via various types of form factors (FFs). In this study, we are going to utilize the recent JLab measurements of the elastic electron-nucleon scattering reduced cross-section, namely GMp12, as a touchstone to unravel the tension observed between the measurements of the WACS cross-section and the data of the proton magnetic F"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2403.19384","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2403.19384/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":"2403.19384","created_at":"2026-07-05T08:14:04.959152+00:00"},{"alias_kind":"arxiv_version","alias_value":"2403.19384v2","created_at":"2026-07-05T08:14:04.959152+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2403.19384","created_at":"2026-07-05T08:14:04.959152+00:00"},{"alias_kind":"pith_short_12","alias_value":"M4GXVVNUX4PG","created_at":"2026-07-05T08:14:04.959152+00:00"},{"alias_kind":"pith_short_16","alias_value":"M4GXVVNUX4PG6UJG","created_at":"2026-07-05T08:14:04.959152+00:00"},{"alias_kind":"pith_short_8","alias_value":"M4GXVVNU","created_at":"2026-07-05T08:14:04.959152+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2601.17948","citing_title":"Tensor form factors of decuplet hyperons in QCD","ref_index":84,"is_internal_anchor":false},{"citing_arxiv_id":"2604.26306","citing_title":"Light sea-quark flavor asymmetry and angular momentum of the nucleon in a scalar-vector spectator model","ref_index":25,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/M4GXVVNUX4PG6UJGEMYYJBLRRG","json":"https://pith.science/pith/M4GXVVNUX4PG6UJGEMYYJBLRRG.json","graph_json":"https://pith.science/api/pith-number/M4GXVVNUX4PG6UJGEMYYJBLRRG/graph.json","events_json":"https://pith.science/api/pith-number/M4GXVVNUX4PG6UJGEMYYJBLRRG/events.json","paper":"https://pith.science/paper/M4GXVVNU"},"agent_actions":{"view_html":"https://pith.science/pith/M4GXVVNUX4PG6UJGEMYYJBLRRG","download_json":"https://pith.science/pith/M4GXVVNUX4PG6UJGEMYYJBLRRG.json","view_paper":"https://pith.science/paper/M4GXVVNU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2403.19384&json=true","fetch_graph":"https://pith.science/api/pith-number/M4GXVVNUX4PG6UJGEMYYJBLRRG/graph.json","fetch_events":"https://pith.science/api/pith-number/M4GXVVNUX4PG6UJGEMYYJBLRRG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/M4GXVVNUX4PG6UJGEMYYJBLRRG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/M4GXVVNUX4PG6UJGEMYYJBLRRG/action/storage_attestation","attest_author":"https://pith.science/pith/M4GXVVNUX4PG6UJGEMYYJBLRRG/action/author_attestation","sign_citation":"https://pith.science/pith/M4GXVVNUX4PG6UJGEMYYJBLRRG/action/citation_signature","submit_replication":"https://pith.science/pith/M4GXVVNUX4PG6UJGEMYYJBLRRG/action/replication_record"}},"created_at":"2026-07-05T08:14:04.959152+00:00","updated_at":"2026-07-05T08:14:04.959152+00:00"}