{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2004:KIWVQBSN2VYNFGN7ZL2JIVP5B6","short_pith_number":"pith:KIWVQBSN","schema_version":"1.0","canonical_sha256":"522d58064dd570d299bfcaf49455fd0fb79f3ca74598b403d624e8b2880508ec","source":{"kind":"arxiv","id":"hep-ph/0403125","version":2},"attestation_state":"computed","paper":{"title":"Pion-Nucleon Scattering Relations at Next-to-Leading Order in 1/N_c","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Abhinav Nellore, Daniel C. Dakin, Richard F. Lebed, Thomas D. Cohen","submitted_at":"2004-03-11T20:43:51Z","abstract_excerpt":"We obtain relations between partial-wave amplitudes for pi-N-->pi-N and pi-N-->pi-Delta directly from large N_c QCD. While linear relations among certain amplitudes holding at leading order (LO) in 1/N_c were derived in the context of chiral soliton models two decades ago, the present work employs a fully model-independent framework based on consistency with the large N_c expansion. At LO we reproduce the soliton model results; however, this method allows for systematic corrections. At next-to-leading order (NLO), most relations require additional unknown functions beyond those appearing at le"},"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/0403125","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2004-03-11T20:43:51Z","cross_cats_sorted":[],"title_canon_sha256":"d0f867f569e3b992d40c033098fc3eb14f352dac0f90e9b0819bf368264e5f38","abstract_canon_sha256":"7fe87caf2d20b0cde431ef4536d1c19723277206bda44f919374c24da995e465"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:48:08.939305Z","signature_b64":"N6W5yAyiVkbZ72geh8otTNa2irnWOwWuw83mB0v7nbYWdpLJgrs5trS3c7BA/XqMbOboO51sstfeyoffm9ZXBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"522d58064dd570d299bfcaf49455fd0fb79f3ca74598b403d624e8b2880508ec","last_reissued_at":"2026-07-04T16:48:08.938967Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:48:08.938967Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Pion-Nucleon Scattering Relations at Next-to-Leading Order in 1/N_c","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Abhinav Nellore, Daniel C. Dakin, Richard F. Lebed, Thomas D. Cohen","submitted_at":"2004-03-11T20:43:51Z","abstract_excerpt":"We obtain relations between partial-wave amplitudes for pi-N-->pi-N and pi-N-->pi-Delta directly from large N_c QCD. While linear relations among certain amplitudes holding at leading order (LO) in 1/N_c were derived in the context of chiral soliton models two decades ago, the present work employs a fully model-independent framework based on consistency with the large N_c expansion. At LO we reproduce the soliton model results; however, this method allows for systematic corrections. At next-to-leading order (NLO), most relations require additional unknown functions beyond those appearing at le"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0403125","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/hep-ph/0403125/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":"hep-ph/0403125","created_at":"2026-07-04T16:48:08.939023+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0403125v2","created_at":"2026-07-04T16:48:08.939023+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0403125","created_at":"2026-07-04T16:48:08.939023+00:00"},{"alias_kind":"pith_short_12","alias_value":"KIWVQBSN2VYN","created_at":"2026-07-04T16:48:08.939023+00:00"},{"alias_kind":"pith_short_16","alias_value":"KIWVQBSN2VYNFGN7","created_at":"2026-07-04T16:48:08.939023+00:00"},{"alias_kind":"pith_short_8","alias_value":"KIWVQBSN","created_at":"2026-07-04T16:48:08.939023+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/KIWVQBSN2VYNFGN7ZL2JIVP5B6","json":"https://pith.science/pith/KIWVQBSN2VYNFGN7ZL2JIVP5B6.json","graph_json":"https://pith.science/api/pith-number/KIWVQBSN2VYNFGN7ZL2JIVP5B6/graph.json","events_json":"https://pith.science/api/pith-number/KIWVQBSN2VYNFGN7ZL2JIVP5B6/events.json","paper":"https://pith.science/paper/KIWVQBSN"},"agent_actions":{"view_html":"https://pith.science/pith/KIWVQBSN2VYNFGN7ZL2JIVP5B6","download_json":"https://pith.science/pith/KIWVQBSN2VYNFGN7ZL2JIVP5B6.json","view_paper":"https://pith.science/paper/KIWVQBSN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0403125&json=true","fetch_graph":"https://pith.science/api/pith-number/KIWVQBSN2VYNFGN7ZL2JIVP5B6/graph.json","fetch_events":"https://pith.science/api/pith-number/KIWVQBSN2VYNFGN7ZL2JIVP5B6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KIWVQBSN2VYNFGN7ZL2JIVP5B6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KIWVQBSN2VYNFGN7ZL2JIVP5B6/action/storage_attestation","attest_author":"https://pith.science/pith/KIWVQBSN2VYNFGN7ZL2JIVP5B6/action/author_attestation","sign_citation":"https://pith.science/pith/KIWVQBSN2VYNFGN7ZL2JIVP5B6/action/citation_signature","submit_replication":"https://pith.science/pith/KIWVQBSN2VYNFGN7ZL2JIVP5B6/action/replication_record"}},"created_at":"2026-07-04T16:48:08.939023+00:00","updated_at":"2026-07-04T16:48:08.939023+00:00"}