{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2009:7COPKZ3X3ITRFZGMMXQ3F3I3IE","short_pith_number":"pith:7COPKZ3X","canonical_record":{"source":{"id":"0908.1758","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-08-12T17:37:46Z","cross_cats_sorted":[],"title_canon_sha256":"6f2e26794981c33bd43eb75c5e6aeac51507abcc8b56688846d0e541df69152c","abstract_canon_sha256":"985a55a45c3449c4b1cee6c430dfb5a8165e9f418d5b98b4f8aa9c5e977b5801"},"schema_version":"1.0"},"canonical_sha256":"f89cf56777da2712e4cc65e1b2ed1b4108b2ce6762d6eee6af84262a462743f6","source":{"kind":"arxiv","id":"0908.1758","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0908.1758","created_at":"2026-05-18T02:12:34Z"},{"alias_kind":"arxiv_version","alias_value":"0908.1758v2","created_at":"2026-05-18T02:12:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0908.1758","created_at":"2026-05-18T02:12:34Z"},{"alias_kind":"pith_short_12","alias_value":"7COPKZ3X3ITR","created_at":"2026-05-18T12:25:58Z"},{"alias_kind":"pith_short_16","alias_value":"7COPKZ3X3ITRFZGM","created_at":"2026-05-18T12:25:58Z"},{"alias_kind":"pith_short_8","alias_value":"7COPKZ3X","created_at":"2026-05-18T12:25:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2009:7COPKZ3X3ITRFZGMMXQ3F3I3IE","target":"record","payload":{"canonical_record":{"source":{"id":"0908.1758","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-08-12T17:37:46Z","cross_cats_sorted":[],"title_canon_sha256":"6f2e26794981c33bd43eb75c5e6aeac51507abcc8b56688846d0e541df69152c","abstract_canon_sha256":"985a55a45c3449c4b1cee6c430dfb5a8165e9f418d5b98b4f8aa9c5e977b5801"},"schema_version":"1.0"},"canonical_sha256":"f89cf56777da2712e4cc65e1b2ed1b4108b2ce6762d6eee6af84262a462743f6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:12:34.902026Z","signature_b64":"CCrhtyDHtjmefS+KHs2eDOhx7oycrxCU16/xLD/WS+vD1hDG7D5NUqzUWK3wJevey/UXPbV1DYQAsJZmI5bzCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f89cf56777da2712e4cc65e1b2ed1b4108b2ce6762d6eee6af84262a462743f6","last_reissued_at":"2026-05-18T02:12:34.901380Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:12:34.901380Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0908.1758","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:12:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PKjqAAGl0Z2xrN5vhm7VAxAE4XXTpONGc42OBSqV3EXGDMSX6vE71baT5VLv/PpMJkoWWLjSv1PH9gnN5BHxBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T18:21:24.535220Z"},"content_sha256":"ffee85a827c51c57775c42bdbda2bf4082bdefb0b89a4c7eaee1b58dd4914e8b","schema_version":"1.0","event_id":"sha256:ffee85a827c51c57775c42bdbda2bf4082bdefb0b89a4c7eaee1b58dd4914e8b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2009:7COPKZ3X3ITRFZGMMXQ3F3I3IE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Semileptonic $\\Lambda_{b,c}$ to Nucleon Transitions in Full QCD at Light Cone","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"H. Sundu, K. Azizi, M. Bayar, Y. Sarac","submitted_at":"2009-08-12T17:37:46Z","abstract_excerpt":"The tree level semileptonic $\\Lambda_{b}\\to pl\\nu$ and $\\Lambda_{c}\\to nl\\nu$ transitions are investigated using the light cone QCD sum rules approach in full theory. The spin--1/2, $\\Lambda_{Q}$ baryon with $Q=b$ or $c$, is considered by the most general form of its interpolating current. The time ordering product of the initial and transition currents is expanded in terms of the nucleon distribution amplitudes with different twists. Considering two sets of independent input parameters entering to the nucleon wave functions, namely, QCD sum rules and Lattice QCD parameters, the related form f"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0908.1758","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:12:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"r59YkMUSLdWstzCb9p6+/9Qks5oVnCfG2JA6t5T/vjSU2CcKqxc3FiYq9v1KX1DDGgaXk10c01nFvYeTgSiVBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T18:21:24.535930Z"},"content_sha256":"e647690944c492155bd91a67ae124da91c2c3d0d42dd8068484418329c3fbcc5","schema_version":"1.0","event_id":"sha256:e647690944c492155bd91a67ae124da91c2c3d0d42dd8068484418329c3fbcc5"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/7COPKZ3X3ITRFZGMMXQ3F3I3IE/bundle.json","state_url":"https://pith.science/pith/7COPKZ3X3ITRFZGMMXQ3F3I3IE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/7COPKZ3X3ITRFZGMMXQ3F3I3IE/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":"2026-05-25T18:21:24Z","links":{"resolver":"https://pith.science/pith/7COPKZ3X3ITRFZGMMXQ3F3I3IE","bundle":"https://pith.science/pith/7COPKZ3X3ITRFZGMMXQ3F3I3IE/bundle.json","state":"https://pith.science/pith/7COPKZ3X3ITRFZGMMXQ3F3I3IE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/7COPKZ3X3ITRFZGMMXQ3F3I3IE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2009:7COPKZ3X3ITRFZGMMXQ3F3I3IE","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":"985a55a45c3449c4b1cee6c430dfb5a8165e9f418d5b98b4f8aa9c5e977b5801","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-08-12T17:37:46Z","title_canon_sha256":"6f2e26794981c33bd43eb75c5e6aeac51507abcc8b56688846d0e541df69152c"},"schema_version":"1.0","source":{"id":"0908.1758","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0908.1758","created_at":"2026-05-18T02:12:34Z"},{"alias_kind":"arxiv_version","alias_value":"0908.1758v2","created_at":"2026-05-18T02:12:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0908.1758","created_at":"2026-05-18T02:12:34Z"},{"alias_kind":"pith_short_12","alias_value":"7COPKZ3X3ITR","created_at":"2026-05-18T12:25:58Z"},{"alias_kind":"pith_short_16","alias_value":"7COPKZ3X3ITRFZGM","created_at":"2026-05-18T12:25:58Z"},{"alias_kind":"pith_short_8","alias_value":"7COPKZ3X","created_at":"2026-05-18T12:25:58Z"}],"graph_snapshots":[{"event_id":"sha256:e647690944c492155bd91a67ae124da91c2c3d0d42dd8068484418329c3fbcc5","target":"graph","created_at":"2026-05-18T02:12:34Z","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 tree level semileptonic $\\Lambda_{b}\\to pl\\nu$ and $\\Lambda_{c}\\to nl\\nu$ transitions are investigated using the light cone QCD sum rules approach in full theory. The spin--1/2, $\\Lambda_{Q}$ baryon with $Q=b$ or $c$, is considered by the most general form of its interpolating current. The time ordering product of the initial and transition currents is expanded in terms of the nucleon distribution amplitudes with different twists. Considering two sets of independent input parameters entering to the nucleon wave functions, namely, QCD sum rules and Lattice QCD parameters, the related form f","authors_text":"H. Sundu, K. Azizi, M. Bayar, Y. Sarac","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-08-12T17:37:46Z","title":"Semileptonic $\\Lambda_{b,c}$ to Nucleon Transitions in Full QCD at Light Cone"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0908.1758","kind":"arxiv","version":2},"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:ffee85a827c51c57775c42bdbda2bf4082bdefb0b89a4c7eaee1b58dd4914e8b","target":"record","created_at":"2026-05-18T02:12:34Z","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":"985a55a45c3449c4b1cee6c430dfb5a8165e9f418d5b98b4f8aa9c5e977b5801","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-08-12T17:37:46Z","title_canon_sha256":"6f2e26794981c33bd43eb75c5e6aeac51507abcc8b56688846d0e541df69152c"},"schema_version":"1.0","source":{"id":"0908.1758","kind":"arxiv","version":2}},"canonical_sha256":"f89cf56777da2712e4cc65e1b2ed1b4108b2ce6762d6eee6af84262a462743f6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f89cf56777da2712e4cc65e1b2ed1b4108b2ce6762d6eee6af84262a462743f6","first_computed_at":"2026-05-18T02:12:34.901380Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:12:34.901380Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"CCrhtyDHtjmefS+KHs2eDOhx7oycrxCU16/xLD/WS+vD1hDG7D5NUqzUWK3wJevey/UXPbV1DYQAsJZmI5bzCg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:12:34.902026Z","signed_message":"canonical_sha256_bytes"},"source_id":"0908.1758","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ffee85a827c51c57775c42bdbda2bf4082bdefb0b89a4c7eaee1b58dd4914e8b","sha256:e647690944c492155bd91a67ae124da91c2c3d0d42dd8068484418329c3fbcc5"],"state_sha256":"33d9fdb693bba24fb5da71ef9babc5f4d78ef817fc99cb7e23eb8e52afc5e238"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"svLAAdBh4FkTAB+60Sy/ZMldhQqO2bw9g/LPBHqb067ljUnDQilR8nRw4JVunCzzyFURhUuVaWOIiygZ6vrNDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T18:21:24.539866Z","bundle_sha256":"970061a6771fcf72a40c9213e2661aced2c13d53a92e59bd10ff4102756f0224"}}