{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:UBUFECO2RU76YZKVFSP3HINRHQ","short_pith_number":"pith:UBUFECO2","schema_version":"1.0","canonical_sha256":"a0685209da8d3fec65552c9fb3a1b13c33e2f77939a67ca45a9fee6a71b2f199","source":{"kind":"arxiv","id":"1501.07218","version":2},"attestation_state":"computed","paper":{"title":"Model-independent calculation of $SU(3)_f$ violation in baryon octet light-cone distribution amplitudes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"Andreas Sch\\\"afer, Philipp Wein","submitted_at":"2015-01-28T18:10:13Z","abstract_excerpt":"In this work we present a minimal parametrization of the light-cone distribution amplitudes of the baryon octet including higher twist contributions. Simultaneously we obtain the quark mass dependence of the amplitudes at leading one-loop accuracy by the use of three-flavor baryon chiral perturbation theory (BChPT), which automatically yields model-independent results for the leading $SU(3)$ flavor breaking effects. For that purpose we have constructed the nonlocal light-cone three-quark operators in terms of baryon octet and meson fields and have carried out a next-to-leading order BChPT calc"},"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":"1501.07218","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-01-28T18:10:13Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"24ae3c2d5e066e660e9be7478a67461413c7aa4984554db5e13eeca779fed829","abstract_canon_sha256":"68dc9794735fd8e656643f8aa86f8dc86c99a1fe34046235ab98c46ca001e6ec"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:26:34.397338Z","signature_b64":"Zl1lNP49COYpzklbpQfAFnfO2CBAJd0IvEETx87p4N7UKzZGfTlkCk+ydATMHT2jEDOjWgeffgRlKITOmgMIAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a0685209da8d3fec65552c9fb3a1b13c33e2f77939a67ca45a9fee6a71b2f199","last_reissued_at":"2026-05-18T01:26:34.396295Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:26:34.396295Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Model-independent calculation of $SU(3)_f$ violation in baryon octet light-cone distribution amplitudes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"Andreas Sch\\\"afer, Philipp Wein","submitted_at":"2015-01-28T18:10:13Z","abstract_excerpt":"In this work we present a minimal parametrization of the light-cone distribution amplitudes of the baryon octet including higher twist contributions. Simultaneously we obtain the quark mass dependence of the amplitudes at leading one-loop accuracy by the use of three-flavor baryon chiral perturbation theory (BChPT), which automatically yields model-independent results for the leading $SU(3)$ flavor breaking effects. For that purpose we have constructed the nonlocal light-cone three-quark operators in terms of baryon octet and meson fields and have carried out a next-to-leading order BChPT calc"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1501.07218","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":""},"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":"1501.07218","created_at":"2026-05-18T01:26:34.396684+00:00"},{"alias_kind":"arxiv_version","alias_value":"1501.07218v2","created_at":"2026-05-18T01:26:34.396684+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1501.07218","created_at":"2026-05-18T01:26:34.396684+00:00"},{"alias_kind":"pith_short_12","alias_value":"UBUFECO2RU76","created_at":"2026-05-18T12:29:44.643036+00:00"},{"alias_kind":"pith_short_16","alias_value":"UBUFECO2RU76YZKV","created_at":"2026-05-18T12:29:44.643036+00:00"},{"alias_kind":"pith_short_8","alias_value":"UBUFECO2","created_at":"2026-05-18T12:29:44.643036+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/UBUFECO2RU76YZKVFSP3HINRHQ","json":"https://pith.science/pith/UBUFECO2RU76YZKVFSP3HINRHQ.json","graph_json":"https://pith.science/api/pith-number/UBUFECO2RU76YZKVFSP3HINRHQ/graph.json","events_json":"https://pith.science/api/pith-number/UBUFECO2RU76YZKVFSP3HINRHQ/events.json","paper":"https://pith.science/paper/UBUFECO2"},"agent_actions":{"view_html":"https://pith.science/pith/UBUFECO2RU76YZKVFSP3HINRHQ","download_json":"https://pith.science/pith/UBUFECO2RU76YZKVFSP3HINRHQ.json","view_paper":"https://pith.science/paper/UBUFECO2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1501.07218&json=true","fetch_graph":"https://pith.science/api/pith-number/UBUFECO2RU76YZKVFSP3HINRHQ/graph.json","fetch_events":"https://pith.science/api/pith-number/UBUFECO2RU76YZKVFSP3HINRHQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UBUFECO2RU76YZKVFSP3HINRHQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UBUFECO2RU76YZKVFSP3HINRHQ/action/storage_attestation","attest_author":"https://pith.science/pith/UBUFECO2RU76YZKVFSP3HINRHQ/action/author_attestation","sign_citation":"https://pith.science/pith/UBUFECO2RU76YZKVFSP3HINRHQ/action/citation_signature","submit_replication":"https://pith.science/pith/UBUFECO2RU76YZKVFSP3HINRHQ/action/replication_record"}},"created_at":"2026-05-18T01:26:34.396684+00:00","updated_at":"2026-05-18T01:26:34.396684+00:00"}