{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:73ZWQ7YOFXEQNRMTQCSY7JXJSZ","short_pith_number":"pith:73ZWQ7YO","canonical_record":{"source":{"id":"1202.4100","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-02-18T20:01:14Z","cross_cats_sorted":[],"title_canon_sha256":"5a96f17d09fb0e3109f4fbebb25bac280a23f416400a0cfe5b00abff1b5ff1d4","abstract_canon_sha256":"af524fb34063889adc6f11db57e27c0b284bb33f9ddb9e9ff7493785eff3f471"},"schema_version":"1.0"},"canonical_sha256":"fef3687f0e2dc906c59380a58fa6e996476c56f974a82db7edde70a09bc7254a","source":{"kind":"arxiv","id":"1202.4100","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1202.4100","created_at":"2026-05-18T01:58:23Z"},{"alias_kind":"arxiv_version","alias_value":"1202.4100v1","created_at":"2026-05-18T01:58:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1202.4100","created_at":"2026-05-18T01:58:23Z"},{"alias_kind":"pith_short_12","alias_value":"73ZWQ7YOFXEQ","created_at":"2026-05-18T12:26:56Z"},{"alias_kind":"pith_short_16","alias_value":"73ZWQ7YOFXEQNRMT","created_at":"2026-05-18T12:26:56Z"},{"alias_kind":"pith_short_8","alias_value":"73ZWQ7YO","created_at":"2026-05-18T12:26:56Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:73ZWQ7YOFXEQNRMTQCSY7JXJSZ","target":"record","payload":{"canonical_record":{"source":{"id":"1202.4100","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-02-18T20:01:14Z","cross_cats_sorted":[],"title_canon_sha256":"5a96f17d09fb0e3109f4fbebb25bac280a23f416400a0cfe5b00abff1b5ff1d4","abstract_canon_sha256":"af524fb34063889adc6f11db57e27c0b284bb33f9ddb9e9ff7493785eff3f471"},"schema_version":"1.0"},"canonical_sha256":"fef3687f0e2dc906c59380a58fa6e996476c56f974a82db7edde70a09bc7254a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:58:23.895598Z","signature_b64":"U+QHf/AJvb96J9hHVdgGw3RXoJNc4vVX2tjqOO0pCO1bKHSobQb+EX+ibBYTO8iOH2RiH1qr80TnZ6FH0HaNDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fef3687f0e2dc906c59380a58fa6e996476c56f974a82db7edde70a09bc7254a","last_reissued_at":"2026-05-18T01:58:23.895115Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:58:23.895115Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1202.4100","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":"2026-05-18T01:58:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rek+F+wZ4bnArMJnH4mn9qUJLrcHjBLHe64wt7aP4sg8jLA4cntyPg95o22G3LK4P4JuBLmNDRuGOnUdADXYCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T13:23:30.151987Z"},"content_sha256":"bb3a7bffdc2b29f64bd182590202325e8cdc7c948921ac197ee563ff2f19d873","schema_version":"1.0","event_id":"sha256:bb3a7bffdc2b29f64bd182590202325e8cdc7c948921ac197ee563ff2f19d873"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:73ZWQ7YOFXEQNRMTQCSY7JXJSZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"New results on the baryon decay Lambda_b -> Lambda_c ell nu in Heavy Quark Effective Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"F. Jugeau, L. Oliver, Yu Jia","submitted_at":"2012-02-18T20:01:14Z","abstract_excerpt":"The baryon differential spectrum of the baryon decay $\\Lambda_b \\to \\Lambda_c \\ell \\bar{\\nu}_\\ell$ will be measured in detail at LHCb. We obtain new results on the form factors in the heavy quark expansion of Heavy Quark Effective Theory that can be useful in the interpretation of the data. We formulate a sum rule for the elastic subleading form factor $A(w)$ at order $1/m_Q$, that originates from the Lagrangian perturbation $\\mathcal{L}_{kin}$. In the sum rule appear only the intermediate states $(j^P, J^P) = (0^+, {1 \\over 2}^+)$, entering also in the $1/{m_Q^2}$ correction to the axial form"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1202.4100","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":"2026-05-18T01:58:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XPe5DTxrnasmxuWz+tv9jTe7TUwxrmHIbZyEtX2llKvd163DoNPm4OPtz2B67yANPxVWW4FaLJMO2zeRj7LuDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T13:23:30.152682Z"},"content_sha256":"ae8e08438f1ae88d4037ffe7c6e0a5eb7208dbf6292865999e6782f366270d1f","schema_version":"1.0","event_id":"sha256:ae8e08438f1ae88d4037ffe7c6e0a5eb7208dbf6292865999e6782f366270d1f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/73ZWQ7YOFXEQNRMTQCSY7JXJSZ/bundle.json","state_url":"https://pith.science/pith/73ZWQ7YOFXEQNRMTQCSY7JXJSZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/73ZWQ7YOFXEQNRMTQCSY7JXJSZ/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":"2026-05-25T13:23:30Z","links":{"resolver":"https://pith.science/pith/73ZWQ7YOFXEQNRMTQCSY7JXJSZ","bundle":"https://pith.science/pith/73ZWQ7YOFXEQNRMTQCSY7JXJSZ/bundle.json","state":"https://pith.science/pith/73ZWQ7YOFXEQNRMTQCSY7JXJSZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/73ZWQ7YOFXEQNRMTQCSY7JXJSZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:73ZWQ7YOFXEQNRMTQCSY7JXJSZ","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":"af524fb34063889adc6f11db57e27c0b284bb33f9ddb9e9ff7493785eff3f471","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-02-18T20:01:14Z","title_canon_sha256":"5a96f17d09fb0e3109f4fbebb25bac280a23f416400a0cfe5b00abff1b5ff1d4"},"schema_version":"1.0","source":{"id":"1202.4100","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1202.4100","created_at":"2026-05-18T01:58:23Z"},{"alias_kind":"arxiv_version","alias_value":"1202.4100v1","created_at":"2026-05-18T01:58:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1202.4100","created_at":"2026-05-18T01:58:23Z"},{"alias_kind":"pith_short_12","alias_value":"73ZWQ7YOFXEQ","created_at":"2026-05-18T12:26:56Z"},{"alias_kind":"pith_short_16","alias_value":"73ZWQ7YOFXEQNRMT","created_at":"2026-05-18T12:26:56Z"},{"alias_kind":"pith_short_8","alias_value":"73ZWQ7YO","created_at":"2026-05-18T12:26:56Z"}],"graph_snapshots":[{"event_id":"sha256:ae8e08438f1ae88d4037ffe7c6e0a5eb7208dbf6292865999e6782f366270d1f","target":"graph","created_at":"2026-05-18T01:58:23Z","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 baryon differential spectrum of the baryon decay $\\Lambda_b \\to \\Lambda_c \\ell \\bar{\\nu}_\\ell$ will be measured in detail at LHCb. We obtain new results on the form factors in the heavy quark expansion of Heavy Quark Effective Theory that can be useful in the interpretation of the data. We formulate a sum rule for the elastic subleading form factor $A(w)$ at order $1/m_Q$, that originates from the Lagrangian perturbation $\\mathcal{L}_{kin}$. In the sum rule appear only the intermediate states $(j^P, J^P) = (0^+, {1 \\over 2}^+)$, entering also in the $1/{m_Q^2}$ correction to the axial form","authors_text":"F. Jugeau, L. Oliver, Yu Jia","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-02-18T20:01:14Z","title":"New results on the baryon decay Lambda_b -> Lambda_c ell nu in Heavy Quark Effective Theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1202.4100","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:bb3a7bffdc2b29f64bd182590202325e8cdc7c948921ac197ee563ff2f19d873","target":"record","created_at":"2026-05-18T01:58:23Z","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":"af524fb34063889adc6f11db57e27c0b284bb33f9ddb9e9ff7493785eff3f471","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-02-18T20:01:14Z","title_canon_sha256":"5a96f17d09fb0e3109f4fbebb25bac280a23f416400a0cfe5b00abff1b5ff1d4"},"schema_version":"1.0","source":{"id":"1202.4100","kind":"arxiv","version":1}},"canonical_sha256":"fef3687f0e2dc906c59380a58fa6e996476c56f974a82db7edde70a09bc7254a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"fef3687f0e2dc906c59380a58fa6e996476c56f974a82db7edde70a09bc7254a","first_computed_at":"2026-05-18T01:58:23.895115Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:58:23.895115Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"U+QHf/AJvb96J9hHVdgGw3RXoJNc4vVX2tjqOO0pCO1bKHSobQb+EX+ibBYTO8iOH2RiH1qr80TnZ6FH0HaNDg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:58:23.895598Z","signed_message":"canonical_sha256_bytes"},"source_id":"1202.4100","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:bb3a7bffdc2b29f64bd182590202325e8cdc7c948921ac197ee563ff2f19d873","sha256:ae8e08438f1ae88d4037ffe7c6e0a5eb7208dbf6292865999e6782f366270d1f"],"state_sha256":"065888ac917719e75545c493d74373b5458fa5dcac465d6ed1c62a4322640497"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IrWf1uBJ4hPyg5Es6FmnZTZVpk7GpuXkpVdCD+0qCYySkFtePBg9Mmbqm0pAg9oeyyeRuykJtt5eU2Whc1nAAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T13:23:30.156905Z","bundle_sha256":"a8e81a46dd8ec2b936aa345e85b343bc91cbd175d73637645a1721556df36f37"}}