{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2000:IET3XJE535LVM2M3JGMLLPBSAK","short_pith_number":"pith:IET3XJE5","schema_version":"1.0","canonical_sha256":"4127bba49ddf5756699b4998b5bc320280a31bc7854a102b935f0b0c531347f7","source":{"kind":"arxiv","id":"nucl-th/0003035","version":1},"attestation_state":"computed","paper":{"title":"Inelastic photon scattering and the magnetic moment of the $\\Delta$ (1232) resonance","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"D. Drechsel, E. Santopinto, M.M. Giannini, M. Vanderhaeghen","submitted_at":"2000-03-15T10:33:59Z","abstract_excerpt":"The reaction $\\gamma+p\\to\\gamma'+p+\\pi^0$ has been suggested as a means to deduce the $\\Delta^+$ magnetic moment. The cross section for this process is estimated in both the constituent quark model and an effective Lagrangian procedure. The resulting total cross section is of the order 5-10 nb, which is at the limit of present experimental capabilities."},"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":"nucl-th/0003035","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2000-03-15T10:33:59Z","cross_cats_sorted":[],"title_canon_sha256":"49532e6e358671b58c867fb5bfd27f2ab9d2eff510223aed645c43a659960ea1","abstract_canon_sha256":"7c64262a0d263be8ed6e3058b4b4b9b37281c0c24830a61549fde64d82a7cae4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:05:21.333934Z","signature_b64":"ZJ1jr0kGfjvM2IcFBAOOTqloFhCnupihGWjxDHQ1sreZvHdS5zCnmnERPNA8GvVTm8ue8QFw5bPO25w73TnHBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4127bba49ddf5756699b4998b5bc320280a31bc7854a102b935f0b0c531347f7","last_reissued_at":"2026-05-18T01:05:21.333472Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:05:21.333472Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Inelastic photon scattering and the magnetic moment of the $\\Delta$ (1232) resonance","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"D. Drechsel, E. Santopinto, M.M. Giannini, M. Vanderhaeghen","submitted_at":"2000-03-15T10:33:59Z","abstract_excerpt":"The reaction $\\gamma+p\\to\\gamma'+p+\\pi^0$ has been suggested as a means to deduce the $\\Delta^+$ magnetic moment. The cross section for this process is estimated in both the constituent quark model and an effective Lagrangian procedure. The resulting total cross section is of the order 5-10 nb, which is at the limit of present experimental capabilities."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0003035","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":""},"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":"nucl-th/0003035","created_at":"2026-05-18T01:05:21.333555+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0003035v1","created_at":"2026-05-18T01:05:21.333555+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0003035","created_at":"2026-05-18T01:05:21.333555+00:00"},{"alias_kind":"pith_short_12","alias_value":"IET3XJE535LV","created_at":"2026-05-18T12:25:49.631198+00:00"},{"alias_kind":"pith_short_16","alias_value":"IET3XJE535LVM2M3","created_at":"2026-05-18T12:25:49.631198+00:00"},{"alias_kind":"pith_short_8","alias_value":"IET3XJE5","created_at":"2026-05-18T12:25:49.631198+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/IET3XJE535LVM2M3JGMLLPBSAK","json":"https://pith.science/pith/IET3XJE535LVM2M3JGMLLPBSAK.json","graph_json":"https://pith.science/api/pith-number/IET3XJE535LVM2M3JGMLLPBSAK/graph.json","events_json":"https://pith.science/api/pith-number/IET3XJE535LVM2M3JGMLLPBSAK/events.json","paper":"https://pith.science/paper/IET3XJE5"},"agent_actions":{"view_html":"https://pith.science/pith/IET3XJE535LVM2M3JGMLLPBSAK","download_json":"https://pith.science/pith/IET3XJE535LVM2M3JGMLLPBSAK.json","view_paper":"https://pith.science/paper/IET3XJE5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/0003035&json=true","fetch_graph":"https://pith.science/api/pith-number/IET3XJE535LVM2M3JGMLLPBSAK/graph.json","fetch_events":"https://pith.science/api/pith-number/IET3XJE535LVM2M3JGMLLPBSAK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IET3XJE535LVM2M3JGMLLPBSAK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IET3XJE535LVM2M3JGMLLPBSAK/action/storage_attestation","attest_author":"https://pith.science/pith/IET3XJE535LVM2M3JGMLLPBSAK/action/author_attestation","sign_citation":"https://pith.science/pith/IET3XJE535LVM2M3JGMLLPBSAK/action/citation_signature","submit_replication":"https://pith.science/pith/IET3XJE535LVM2M3JGMLLPBSAK/action/replication_record"}},"created_at":"2026-05-18T01:05:21.333555+00:00","updated_at":"2026-05-18T01:05:21.333555+00:00"}