{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:3U4T35BCLQRTQRCAYXZIUSSJH5","short_pith_number":"pith:3U4T35BC","schema_version":"1.0","canonical_sha256":"dd393df4225c23384440c5f28a4a493f715c83b7203aa56aced76cce710db150","source":{"kind":"arxiv","id":"0904.4894","version":1},"attestation_state":"computed","paper":{"title":"SU(3)-breaking corrections to the baryon-octet magnetic moments in chiral perturbation theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"J. Martin Camalich, L. Alvarez-Ruso, L.S. Geng, M.J. Vicente Vacas","submitted_at":"2009-04-30T17:24:00Z","abstract_excerpt":"We report a calculation of the baryon magnetic moments using covariant chiral perturbation theory within the extended-on-mass-shell renormalization scheme including intermediate octet and decuplet contributions. By fitting the two available low-energy constants, we improve the Coleman-Glashow description of the data when we include the leading SU(3) breaking effects coming from the lowest-order loops. We compare with previous attempts at the same order using heavy-baryon and covariant infrared chiral perturbation theory, and discuss the source of the differences."},"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":"0904.4894","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-04-30T17:24:00Z","cross_cats_sorted":[],"title_canon_sha256":"2a513fc334d508a516c1b61e11477a630d62c4c5f5c9bb8e3beb9192d4f20249","abstract_canon_sha256":"67a336faa4ace8e1974eb8a6d73016f12afe0db247917b5f6bce7f84be50dd84"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:29:54.079898Z","signature_b64":"nZvXVKa5J5LbFHclu5cB0iOKAGZPJD22asZoDMHAEuuhGeeRpkLqu95LwPN3+Zvz9JP2JdidVZZkRe7War2+Dw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dd393df4225c23384440c5f28a4a493f715c83b7203aa56aced76cce710db150","last_reissued_at":"2026-05-18T04:29:54.079166Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:29:54.079166Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"SU(3)-breaking corrections to the baryon-octet magnetic moments in chiral perturbation theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"J. Martin Camalich, L. Alvarez-Ruso, L.S. Geng, M.J. Vicente Vacas","submitted_at":"2009-04-30T17:24:00Z","abstract_excerpt":"We report a calculation of the baryon magnetic moments using covariant chiral perturbation theory within the extended-on-mass-shell renormalization scheme including intermediate octet and decuplet contributions. By fitting the two available low-energy constants, we improve the Coleman-Glashow description of the data when we include the leading SU(3) breaking effects coming from the lowest-order loops. We compare with previous attempts at the same order using heavy-baryon and covariant infrared chiral perturbation theory, and discuss the source of the differences."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0904.4894","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":"0904.4894","created_at":"2026-05-18T04:29:54.079241+00:00"},{"alias_kind":"arxiv_version","alias_value":"0904.4894v1","created_at":"2026-05-18T04:29:54.079241+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0904.4894","created_at":"2026-05-18T04:29:54.079241+00:00"},{"alias_kind":"pith_short_12","alias_value":"3U4T35BCLQRT","created_at":"2026-05-18T12:25:58.018023+00:00"},{"alias_kind":"pith_short_16","alias_value":"3U4T35BCLQRTQRCA","created_at":"2026-05-18T12:25:58.018023+00:00"},{"alias_kind":"pith_short_8","alias_value":"3U4T35BC","created_at":"2026-05-18T12:25:58.018023+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/3U4T35BCLQRTQRCAYXZIUSSJH5","json":"https://pith.science/pith/3U4T35BCLQRTQRCAYXZIUSSJH5.json","graph_json":"https://pith.science/api/pith-number/3U4T35BCLQRTQRCAYXZIUSSJH5/graph.json","events_json":"https://pith.science/api/pith-number/3U4T35BCLQRTQRCAYXZIUSSJH5/events.json","paper":"https://pith.science/paper/3U4T35BC"},"agent_actions":{"view_html":"https://pith.science/pith/3U4T35BCLQRTQRCAYXZIUSSJH5","download_json":"https://pith.science/pith/3U4T35BCLQRTQRCAYXZIUSSJH5.json","view_paper":"https://pith.science/paper/3U4T35BC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0904.4894&json=true","fetch_graph":"https://pith.science/api/pith-number/3U4T35BCLQRTQRCAYXZIUSSJH5/graph.json","fetch_events":"https://pith.science/api/pith-number/3U4T35BCLQRTQRCAYXZIUSSJH5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3U4T35BCLQRTQRCAYXZIUSSJH5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3U4T35BCLQRTQRCAYXZIUSSJH5/action/storage_attestation","attest_author":"https://pith.science/pith/3U4T35BCLQRTQRCAYXZIUSSJH5/action/author_attestation","sign_citation":"https://pith.science/pith/3U4T35BCLQRTQRCAYXZIUSSJH5/action/citation_signature","submit_replication":"https://pith.science/pith/3U4T35BCLQRTQRCAYXZIUSSJH5/action/replication_record"}},"created_at":"2026-05-18T04:29:54.079241+00:00","updated_at":"2026-05-18T04:29:54.079241+00:00"}