{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1999:TRBF66XATJEJF7XLZP4XEKE7QN","short_pith_number":"pith:TRBF66XA","canonical_record":{"source":{"id":"hep-ph/9910342","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1999-10-14T16:02:25Z","cross_cats_sorted":[],"title_canon_sha256":"eeda8d02ecc207a8b6d3e10e7c60cc8aff88f6eeeae965e3ba20ca7e6e43bf90","abstract_canon_sha256":"f95230ec124f34eb43a47be9fbc4956788f21e51c33434eee8f15336b1a0ae35"},"schema_version":"1.0"},"canonical_sha256":"9c425f7ae09a4892feebcbf972289f835f9d4400fcd73932f18145bb9d4534f7","source":{"kind":"arxiv","id":"hep-ph/9910342","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9910342","created_at":"2026-05-18T04:31:00Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9910342v1","created_at":"2026-05-18T04:31:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9910342","created_at":"2026-05-18T04:31:00Z"},{"alias_kind":"pith_short_12","alias_value":"TRBF66XATJEJ","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_16","alias_value":"TRBF66XATJEJF7XL","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_8","alias_value":"TRBF66XA","created_at":"2026-05-18T12:25:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1999:TRBF66XATJEJF7XLZP4XEKE7QN","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9910342","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1999-10-14T16:02:25Z","cross_cats_sorted":[],"title_canon_sha256":"eeda8d02ecc207a8b6d3e10e7c60cc8aff88f6eeeae965e3ba20ca7e6e43bf90","abstract_canon_sha256":"f95230ec124f34eb43a47be9fbc4956788f21e51c33434eee8f15336b1a0ae35"},"schema_version":"1.0"},"canonical_sha256":"9c425f7ae09a4892feebcbf972289f835f9d4400fcd73932f18145bb9d4534f7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:31:00.463635Z","signature_b64":"1VLyCzT4hjdZU31eamt60qgkq1YOMjqxZacRIMSzdgdxm4Fvo0DdAjIMSycufcU042dra34fHvzHjS4BVIqnAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9c425f7ae09a4892feebcbf972289f835f9d4400fcd73932f18145bb9d4534f7","last_reissued_at":"2026-05-18T04:31:00.462907Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:31:00.462907Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9910342","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":"2026-05-18T04:31:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rbKgC3egh6/p79YLMsgZ4XxArov1OsLqHGhO6qoZIQhrXTf0HEiz5ebm5z67TDBg22hYaf23LvGvG6xlE82qCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T01:43:00.543129Z"},"content_sha256":"012b6ad8e47fcffda4f6bb3934ce7f549bfc9cd97c524c2f5dba5b92346a5d53","schema_version":"1.0","event_id":"sha256:012b6ad8e47fcffda4f6bb3934ce7f549bfc9cd97c524c2f5dba5b92346a5d53"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1999:TRBF66XATJEJF7XLZP4XEKE7QN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Lambda_b and Lambda_c baryon decays at finite values of heavy quark masses","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. G. Rusetsky (Bern University, Dubna, Dubna), J. G. Korner (Mainz University), JINR, M. A. Ivanov (JINR, Tbilisi University), Tomsk University), V. E. Lyubovitskij (JINR","submitted_at":"1999-10-14T16:02:25Z","abstract_excerpt":"Semileptonic decays of Lambda_b and Lambda_c baryons are studied within the Relativistic Three-Quark Model using finite heavy quark mass values. Employing the same parameters as have been used previously for the description of exclusive decays of heavy baryons in the heavy quark limit we calculate the six form factors of the process and the corresponding decay rates. Our calculation shows that the ``finite mass'' corrections are important in heavy-to-light transitions and are not negligible in heavy-to-heavy transitions."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9910342","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":"2026-05-18T04:31:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RYv41dnv4Zn/oFf5Qck1f7z0TmDJtFpxApThb3ncerGtmhgAQ3p59MZJLo6moK9ZqTIguo1mr019DKG8MS1EDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T01:43:00.543851Z"},"content_sha256":"f627868c870b033d77258abd182fedb2681e1c4a1c147771604adc1d17a66bfc","schema_version":"1.0","event_id":"sha256:f627868c870b033d77258abd182fedb2681e1c4a1c147771604adc1d17a66bfc"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/TRBF66XATJEJF7XLZP4XEKE7QN/bundle.json","state_url":"https://pith.science/pith/TRBF66XATJEJF7XLZP4XEKE7QN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/TRBF66XATJEJF7XLZP4XEKE7QN/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":"2026-05-26T01:43:00Z","links":{"resolver":"https://pith.science/pith/TRBF66XATJEJF7XLZP4XEKE7QN","bundle":"https://pith.science/pith/TRBF66XATJEJF7XLZP4XEKE7QN/bundle.json","state":"https://pith.science/pith/TRBF66XATJEJF7XLZP4XEKE7QN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/TRBF66XATJEJF7XLZP4XEKE7QN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1999:TRBF66XATJEJF7XLZP4XEKE7QN","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":"f95230ec124f34eb43a47be9fbc4956788f21e51c33434eee8f15336b1a0ae35","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1999-10-14T16:02:25Z","title_canon_sha256":"eeda8d02ecc207a8b6d3e10e7c60cc8aff88f6eeeae965e3ba20ca7e6e43bf90"},"schema_version":"1.0","source":{"id":"hep-ph/9910342","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9910342","created_at":"2026-05-18T04:31:00Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9910342v1","created_at":"2026-05-18T04:31:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9910342","created_at":"2026-05-18T04:31:00Z"},{"alias_kind":"pith_short_12","alias_value":"TRBF66XATJEJ","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_16","alias_value":"TRBF66XATJEJF7XL","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_8","alias_value":"TRBF66XA","created_at":"2026-05-18T12:25:49Z"}],"graph_snapshots":[{"event_id":"sha256:f627868c870b033d77258abd182fedb2681e1c4a1c147771604adc1d17a66bfc","target":"graph","created_at":"2026-05-18T04:31:00Z","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":"Semileptonic decays of Lambda_b and Lambda_c baryons are studied within the Relativistic Three-Quark Model using finite heavy quark mass values. Employing the same parameters as have been used previously for the description of exclusive decays of heavy baryons in the heavy quark limit we calculate the six form factors of the process and the corresponding decay rates. Our calculation shows that the ``finite mass'' corrections are important in heavy-to-light transitions and are not negligible in heavy-to-heavy transitions.","authors_text":"A. G. Rusetsky (Bern University, Dubna, Dubna), J. G. Korner (Mainz University), JINR, M. A. Ivanov (JINR, Tbilisi University), Tomsk University), V. E. Lyubovitskij (JINR","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1999-10-14T16:02:25Z","title":"Lambda_b and Lambda_c baryon decays at finite values of heavy quark masses"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9910342","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":"sha256:012b6ad8e47fcffda4f6bb3934ce7f549bfc9cd97c524c2f5dba5b92346a5d53","target":"record","created_at":"2026-05-18T04:31:00Z","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":"f95230ec124f34eb43a47be9fbc4956788f21e51c33434eee8f15336b1a0ae35","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1999-10-14T16:02:25Z","title_canon_sha256":"eeda8d02ecc207a8b6d3e10e7c60cc8aff88f6eeeae965e3ba20ca7e6e43bf90"},"schema_version":"1.0","source":{"id":"hep-ph/9910342","kind":"arxiv","version":1}},"canonical_sha256":"9c425f7ae09a4892feebcbf972289f835f9d4400fcd73932f18145bb9d4534f7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9c425f7ae09a4892feebcbf972289f835f9d4400fcd73932f18145bb9d4534f7","first_computed_at":"2026-05-18T04:31:00.462907Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:31:00.462907Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"1VLyCzT4hjdZU31eamt60qgkq1YOMjqxZacRIMSzdgdxm4Fvo0DdAjIMSycufcU042dra34fHvzHjS4BVIqnAw==","signature_status":"signed_v1","signed_at":"2026-05-18T04:31:00.463635Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9910342","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:012b6ad8e47fcffda4f6bb3934ce7f549bfc9cd97c524c2f5dba5b92346a5d53","sha256:f627868c870b033d77258abd182fedb2681e1c4a1c147771604adc1d17a66bfc"],"state_sha256":"9837c102dedfcd18c939a6344bf095bbd4a52166c6356e7a7d25b40564370e52"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8tMXSnuIZvqQH9FY7tLj3Fs25sTTl/De9PLQpDhG7h02O7DyU/G+tJffczLOqGVLR07zlrygRpENxcYZ9i9ZCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T01:43:00.547081Z","bundle_sha256":"33d069164e9ad782330ff6e3f1f2aa40fdca2fbe4d8573c3f978e9cdeee98523"}}