{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1996:27MECW7MEZHK3VCDL3KDNOP2BR","short_pith_number":"pith:27MECW7M","canonical_record":{"source":{"id":"hep-ph/9612463","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1996-12-24T17:31:03Z","cross_cats_sorted":[],"title_canon_sha256":"f807bb8fb38137df7f22cb3767f1b061e3f3cdb9d4411a5b72dcef48b757c777","abstract_canon_sha256":"be72bb35a9161f0f8c2ba96151d6211d79964af9c5216d475fa1733b68e2a0d2"},"schema_version":"1.0"},"canonical_sha256":"d7d8415bec264eadd4435ed436b9fa0c6a6bc4a889b7f5a6f3419b97a09c0730","source":{"kind":"arxiv","id":"hep-ph/9612463","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9612463","created_at":"2026-07-04T16:02:01Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9612463v1","created_at":"2026-07-04T16:02:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9612463","created_at":"2026-07-04T16:02:01Z"},{"alias_kind":"pith_short_12","alias_value":"27MECW7MEZHK","created_at":"2026-07-04T16:02:01Z"},{"alias_kind":"pith_short_16","alias_value":"27MECW7MEZHK3VCD","created_at":"2026-07-04T16:02:01Z"},{"alias_kind":"pith_short_8","alias_value":"27MECW7M","created_at":"2026-07-04T16:02:01Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1996:27MECW7MEZHK3VCDL3KDNOP2BR","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9612463","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1996-12-24T17:31:03Z","cross_cats_sorted":[],"title_canon_sha256":"f807bb8fb38137df7f22cb3767f1b061e3f3cdb9d4411a5b72dcef48b757c777","abstract_canon_sha256":"be72bb35a9161f0f8c2ba96151d6211d79964af9c5216d475fa1733b68e2a0d2"},"schema_version":"1.0"},"canonical_sha256":"d7d8415bec264eadd4435ed436b9fa0c6a6bc4a889b7f5a6f3419b97a09c0730","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:02:01.905593Z","signature_b64":"QAh/1T/gJME0gB/rFPQ17Z4d2vj9W5CkdOPE48pSXTr/1ygHIZBa5q1hV7y6Bmhv6ixEUsifBUghq2s0OGwKBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d7d8415bec264eadd4435ed436b9fa0c6a6bc4a889b7f5a6f3419b97a09c0730","last_reissued_at":"2026-07-04T16:02:01.905186Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:02:01.905186Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9612463","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":"2026-07-04T16:02:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AbNwLa0Vwhz1JuJvpn/VviVeyC+JrDF5v8Jv1oC4uaUTgNzlSrbY1xf1BqgfnTh+JqD+pY5WNoikDZxopA/2Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T09:34:16.901032Z"},"content_sha256":"729ff340419863494a19826116af09b4672a3017735d9c57a7dc952729ead060","schema_version":"1.0","event_id":"sha256:729ff340419863494a19826116af09b4672a3017735d9c57a7dc952729ead060"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1996:27MECW7MEZHK3VCDL3KDNOP2BR","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Heavy Baryon Transitions in a Relativistic Three-Quark Model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Dubna), Dubna & Tomsk Uni.), Inst. Phys.), J.G.Korner (Mainz Uni., M.A.Ivanov (JINR, P.Kroll (Wuppertal Uni.), V.E.Lyubovitskij (JINR","submitted_at":"1996-12-24T17:31:03Z","abstract_excerpt":"Exclusive semileptonic decays of bottom and charm baryons are considered within a relativistic three-quark model with a Gaussian shape for the baryon-three-quark vertex and standard quark propagators. We calculate the baryonic Isgur-Wise functions, decay rates and asymmetry parameters."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9612463","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/9612463/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T16:02:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"R3WmZcnKoloSAHP4rw6C22DpiTSQbxeRDX7Ck2Kr/XpobjnZH1hdsa0GQ5oP0qd4FD85pLcdZli4Ue9MbaIcCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T09:34:16.902052Z"},"content_sha256":"241453903f11095488fb6062a7c9ff8d585dec9899da5ce3f2379c635b6ac874","schema_version":"1.0","event_id":"sha256:241453903f11095488fb6062a7c9ff8d585dec9899da5ce3f2379c635b6ac874"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/27MECW7MEZHK3VCDL3KDNOP2BR/bundle.json","state_url":"https://pith.science/pith/27MECW7MEZHK3VCDL3KDNOP2BR/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/27MECW7MEZHK3VCDL3KDNOP2BR/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":"2026-08-06T09:34:16Z","links":{"resolver":"https://pith.science/pith/27MECW7MEZHK3VCDL3KDNOP2BR","bundle":"https://pith.science/pith/27MECW7MEZHK3VCDL3KDNOP2BR/bundle.json","state":"https://pith.science/pith/27MECW7MEZHK3VCDL3KDNOP2BR/state.json","well_known_bundle":"https://pith.science/.well-known/pith/27MECW7MEZHK3VCDL3KDNOP2BR/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1996:27MECW7MEZHK3VCDL3KDNOP2BR","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":"be72bb35a9161f0f8c2ba96151d6211d79964af9c5216d475fa1733b68e2a0d2","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1996-12-24T17:31:03Z","title_canon_sha256":"f807bb8fb38137df7f22cb3767f1b061e3f3cdb9d4411a5b72dcef48b757c777"},"schema_version":"1.0","source":{"id":"hep-ph/9612463","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9612463","created_at":"2026-07-04T16:02:01Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9612463v1","created_at":"2026-07-04T16:02:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9612463","created_at":"2026-07-04T16:02:01Z"},{"alias_kind":"pith_short_12","alias_value":"27MECW7MEZHK","created_at":"2026-07-04T16:02:01Z"},{"alias_kind":"pith_short_16","alias_value":"27MECW7MEZHK3VCD","created_at":"2026-07-04T16:02:01Z"},{"alias_kind":"pith_short_8","alias_value":"27MECW7M","created_at":"2026-07-04T16:02:01Z"}],"graph_snapshots":[{"event_id":"sha256:241453903f11095488fb6062a7c9ff8d585dec9899da5ce3f2379c635b6ac874","target":"graph","created_at":"2026-07-04T16:02:01Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-ph/9612463/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Exclusive semileptonic decays of bottom and charm baryons are considered within a relativistic three-quark model with a Gaussian shape for the baryon-three-quark vertex and standard quark propagators. We calculate the baryonic Isgur-Wise functions, decay rates and asymmetry parameters.","authors_text":"Dubna), Dubna & Tomsk Uni.), Inst. Phys.), J.G.Korner (Mainz Uni., M.A.Ivanov (JINR, P.Kroll (Wuppertal Uni.), V.E.Lyubovitskij (JINR","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1996-12-24T17:31:03Z","title":"Heavy Baryon Transitions in a Relativistic Three-Quark Model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9612463","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":"sha256:729ff340419863494a19826116af09b4672a3017735d9c57a7dc952729ead060","target":"record","created_at":"2026-07-04T16:02:01Z","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":"be72bb35a9161f0f8c2ba96151d6211d79964af9c5216d475fa1733b68e2a0d2","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1996-12-24T17:31:03Z","title_canon_sha256":"f807bb8fb38137df7f22cb3767f1b061e3f3cdb9d4411a5b72dcef48b757c777"},"schema_version":"1.0","source":{"id":"hep-ph/9612463","kind":"arxiv","version":1}},"canonical_sha256":"d7d8415bec264eadd4435ed436b9fa0c6a6bc4a889b7f5a6f3419b97a09c0730","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d7d8415bec264eadd4435ed436b9fa0c6a6bc4a889b7f5a6f3419b97a09c0730","first_computed_at":"2026-07-04T16:02:01.905186Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:02:01.905186Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"QAh/1T/gJME0gB/rFPQ17Z4d2vj9W5CkdOPE48pSXTr/1ygHIZBa5q1hV7y6Bmhv6ixEUsifBUghq2s0OGwKBg==","signature_status":"signed_v1","signed_at":"2026-07-04T16:02:01.905593Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9612463","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:729ff340419863494a19826116af09b4672a3017735d9c57a7dc952729ead060","sha256:241453903f11095488fb6062a7c9ff8d585dec9899da5ce3f2379c635b6ac874"],"state_sha256":"97d8d363d19fd7f9d8f82565dc4706e7411f6da74da6e482f8e09b251a78523d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4c20b1Pp01AJTZCsveVLmbxID0AEf3YyxZZCsVsh/8+S8MORwoVnYj71kTLPuqS/TqLBFNHWGLQDEQpRiHPSCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-06T09:34:16.908058Z","bundle_sha256":"93031056138e381c4b4f1fc6abaaac376ca97a3f346dfa88e7ed5283ab24a89e"}}