{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:4J3WOOVQD3R5TCJAREGLW54IMD","short_pith_number":"pith:4J3WOOVQ","canonical_record":{"source":{"id":"1405.5456","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-05-21T15:26:29Z","cross_cats_sorted":[],"title_canon_sha256":"fb062a41bfbc3a391a4e1f1f224f4db7dab36ff91dea187e196d379e9c01405c","abstract_canon_sha256":"945d49757776453d293af190461337abdb2bad1b6381aa6d951f714d05816f03"},"schema_version":"1.0"},"canonical_sha256":"e277673ab01ee3d98920890cbb778860f30f078639849e8f641673b4fb040a21","source":{"kind":"arxiv","id":"1405.5456","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1405.5456","created_at":"2026-05-18T02:43:10Z"},{"alias_kind":"arxiv_version","alias_value":"1405.5456v1","created_at":"2026-05-18T02:43:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1405.5456","created_at":"2026-05-18T02:43:10Z"},{"alias_kind":"pith_short_12","alias_value":"4J3WOOVQD3R5","created_at":"2026-05-18T12:28:14Z"},{"alias_kind":"pith_short_16","alias_value":"4J3WOOVQD3R5TCJA","created_at":"2026-05-18T12:28:14Z"},{"alias_kind":"pith_short_8","alias_value":"4J3WOOVQ","created_at":"2026-05-18T12:28:14Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:4J3WOOVQD3R5TCJAREGLW54IMD","target":"record","payload":{"canonical_record":{"source":{"id":"1405.5456","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-05-21T15:26:29Z","cross_cats_sorted":[],"title_canon_sha256":"fb062a41bfbc3a391a4e1f1f224f4db7dab36ff91dea187e196d379e9c01405c","abstract_canon_sha256":"945d49757776453d293af190461337abdb2bad1b6381aa6d951f714d05816f03"},"schema_version":"1.0"},"canonical_sha256":"e277673ab01ee3d98920890cbb778860f30f078639849e8f641673b4fb040a21","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:43:10.838675Z","signature_b64":"SoUAgYHeSbQOy2g8U9GyndQmgEBKVW346NSo+HMjazdudQjN5qBdAdFcLM4/V2Oizpc7/LLEXjAT4UC2ie6HCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e277673ab01ee3d98920890cbb778860f30f078639849e8f641673b4fb040a21","last_reissued_at":"2026-05-18T02:43:10.838260Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:43:10.838260Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1405.5456","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:43:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xunEa26YoGiTkBFbkvn7V59JCVYB6py5+67eOSU2OFCS0hua/N0Q9NUZg2/2by1S+wpgXzd4PP0BT6pZpW98Bg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T11:57:16.073989Z"},"content_sha256":"79436cb8f3cbbb181f169599ddb40136efbeae25069a21f90c0258a6c9ecb1ad","schema_version":"1.0","event_id":"sha256:79436cb8f3cbbb181f169599ddb40136efbeae25069a21f90c0258a6c9ecb1ad"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:4J3WOOVQD3R5TCJAREGLW54IMD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Octet-baryon axial-vector charges and SU(3)-breaking effects in the semileptonic hyperon decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"J. Martin Camalich, L. S. Geng, M. J. Vicente Vacas, T. Ledwig","submitted_at":"2014-05-21T15:26:29Z","abstract_excerpt":"The octet-baryon axial-vector charges and the g1/f1 ratios measured in the semileptonic hyperon decays are studied up to O(p^3) using the covariant baryon chiral perturbation theory with explicit decuplet contributions. We clarify the role of different low-energy constants and find a good convergence for the chiral expansion of the axial-vector charges of the baryon octet, g1(0), with O(p^3) corrections typically around 20% of the leading ones. This is a consequence of strong cancellations between different next-to-leading order terms. We show that considering only non-analytic terms is not en"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1405.5456","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:43:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Iat+q2wTKkpg8g4bNzqfoZ8loCHiLlP0tAtymA76DaVNpUod+xC4VCOSipl+1fUaasmhCpchc7CsxQkdFl/IDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T11:57:16.074364Z"},"content_sha256":"5555242795cd512569a5309da5f7da97a238e31c6c33b6d5a73c7dd3f107f534","schema_version":"1.0","event_id":"sha256:5555242795cd512569a5309da5f7da97a238e31c6c33b6d5a73c7dd3f107f534"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4J3WOOVQD3R5TCJAREGLW54IMD/bundle.json","state_url":"https://pith.science/pith/4J3WOOVQD3R5TCJAREGLW54IMD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4J3WOOVQD3R5TCJAREGLW54IMD/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-11T11:57:16Z","links":{"resolver":"https://pith.science/pith/4J3WOOVQD3R5TCJAREGLW54IMD","bundle":"https://pith.science/pith/4J3WOOVQD3R5TCJAREGLW54IMD/bundle.json","state":"https://pith.science/pith/4J3WOOVQD3R5TCJAREGLW54IMD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4J3WOOVQD3R5TCJAREGLW54IMD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:4J3WOOVQD3R5TCJAREGLW54IMD","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"945d49757776453d293af190461337abdb2bad1b6381aa6d951f714d05816f03","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-05-21T15:26:29Z","title_canon_sha256":"fb062a41bfbc3a391a4e1f1f224f4db7dab36ff91dea187e196d379e9c01405c"},"schema_version":"1.0","source":{"id":"1405.5456","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1405.5456","created_at":"2026-05-18T02:43:10Z"},{"alias_kind":"arxiv_version","alias_value":"1405.5456v1","created_at":"2026-05-18T02:43:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1405.5456","created_at":"2026-05-18T02:43:10Z"},{"alias_kind":"pith_short_12","alias_value":"4J3WOOVQD3R5","created_at":"2026-05-18T12:28:14Z"},{"alias_kind":"pith_short_16","alias_value":"4J3WOOVQD3R5TCJA","created_at":"2026-05-18T12:28:14Z"},{"alias_kind":"pith_short_8","alias_value":"4J3WOOVQ","created_at":"2026-05-18T12:28:14Z"}],"graph_snapshots":[{"event_id":"sha256:5555242795cd512569a5309da5f7da97a238e31c6c33b6d5a73c7dd3f107f534","target":"graph","created_at":"2026-05-18T02:43:10Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"The octet-baryon axial-vector charges and the g1/f1 ratios measured in the semileptonic hyperon decays are studied up to O(p^3) using the covariant baryon chiral perturbation theory with explicit decuplet contributions. We clarify the role of different low-energy constants and find a good convergence for the chiral expansion of the axial-vector charges of the baryon octet, g1(0), with O(p^3) corrections typically around 20% of the leading ones. This is a consequence of strong cancellations between different next-to-leading order terms. We show that considering only non-analytic terms is not en","authors_text":"J. Martin Camalich, L. S. Geng, M. J. Vicente Vacas, T. Ledwig","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-05-21T15:26:29Z","title":"Octet-baryon axial-vector charges and SU(3)-breaking effects in the semileptonic hyperon decays"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1405.5456","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:79436cb8f3cbbb181f169599ddb40136efbeae25069a21f90c0258a6c9ecb1ad","target":"record","created_at":"2026-05-18T02:43:10Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"945d49757776453d293af190461337abdb2bad1b6381aa6d951f714d05816f03","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-05-21T15:26:29Z","title_canon_sha256":"fb062a41bfbc3a391a4e1f1f224f4db7dab36ff91dea187e196d379e9c01405c"},"schema_version":"1.0","source":{"id":"1405.5456","kind":"arxiv","version":1}},"canonical_sha256":"e277673ab01ee3d98920890cbb778860f30f078639849e8f641673b4fb040a21","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e277673ab01ee3d98920890cbb778860f30f078639849e8f641673b4fb040a21","first_computed_at":"2026-05-18T02:43:10.838260Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:43:10.838260Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"SoUAgYHeSbQOy2g8U9GyndQmgEBKVW346NSo+HMjazdudQjN5qBdAdFcLM4/V2Oizpc7/LLEXjAT4UC2ie6HCw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:43:10.838675Z","signed_message":"canonical_sha256_bytes"},"source_id":"1405.5456","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:79436cb8f3cbbb181f169599ddb40136efbeae25069a21f90c0258a6c9ecb1ad","sha256:5555242795cd512569a5309da5f7da97a238e31c6c33b6d5a73c7dd3f107f534"],"state_sha256":"ac01f070d125dcce3910fa1c3c8b95f7a628152ec063ec2621c523b129d63f88"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qhGEfkCzzjYU0oVQE/L3FrPTw7OjgbQKvJJpPpFZVa/wypUBbujxPWsket634Pd0BgJF9iy9Ah48ioMOYUCbDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-11T11:57:16.076307Z","bundle_sha256":"fa18ed3cccb34fbff8e10582e849a42d621d355a53122c79c797088e5043dbe8"}}