{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2004:6XGCORNIJMMPLJY35CPC6D4ZTQ","short_pith_number":"pith:6XGCORNI","canonical_record":{"source":{"id":"hep-ph/0402094","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2004-02-09T21:10:18Z","cross_cats_sorted":[],"title_canon_sha256":"88ca89469955f7b5aea6e20ac125521343ca271f44ebd950c089a6ed363d559f","abstract_canon_sha256":"de3aa6f27070024d37ec5dfb69a42f0d0112539cca602fd8e5fbb6d333ad1caf"},"schema_version":"1.0"},"canonical_sha256":"f5cc2745a84b18f5a71be89e2f0f999c3c266d193f87295522c50fd232d5aa81","source":{"kind":"arxiv","id":"hep-ph/0402094","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0402094","created_at":"2026-07-04T16:48:06Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0402094v3","created_at":"2026-07-04T16:48:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0402094","created_at":"2026-07-04T16:48:06Z"},{"alias_kind":"pith_short_12","alias_value":"6XGCORNIJMMP","created_at":"2026-07-04T16:48:06Z"},{"alias_kind":"pith_short_16","alias_value":"6XGCORNIJMMPLJY3","created_at":"2026-07-04T16:48:06Z"},{"alias_kind":"pith_short_8","alias_value":"6XGCORNI","created_at":"2026-07-04T16:48:06Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2004:6XGCORNIJMMPLJY35CPC6D4ZTQ","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0402094","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2004-02-09T21:10:18Z","cross_cats_sorted":[],"title_canon_sha256":"88ca89469955f7b5aea6e20ac125521343ca271f44ebd950c089a6ed363d559f","abstract_canon_sha256":"de3aa6f27070024d37ec5dfb69a42f0d0112539cca602fd8e5fbb6d333ad1caf"},"schema_version":"1.0"},"canonical_sha256":"f5cc2745a84b18f5a71be89e2f0f999c3c266d193f87295522c50fd232d5aa81","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:48:06.599942Z","signature_b64":"86YnIZtggADUWKreM1BtcDrHLQS4aAzsmZ56xgm0LFJvWs59UyggKXjSLaphqB/kgHr0KYVBVzYg80lQSUcNDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f5cc2745a84b18f5a71be89e2f0f999c3c266d193f87295522c50fd232d5aa81","last_reissued_at":"2026-07-04T16:48:06.599574Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:48:06.599574Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0402094","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T16:48:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7GG46uzNrh+qXOKWSBKCP53fJv7XuZsdOkQvK4JKT7l9UPP6aCIdkqzAUZI4qJNDnVmmFjNWkNfZWc4AQnUuAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-02T18:30:02.805537Z"},"content_sha256":"224ae5630aa8ee7f325787fa4c013489df9cce3f04ff20e32dbb5b050d1b043b","schema_version":"1.0","event_id":"sha256:224ae5630aa8ee7f325787fa4c013489df9cce3f04ff20e32dbb5b050d1b043b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2004:6XGCORNIJMMPLJY35CPC6D4ZTQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Factorization and Shape-Function Effects in Inclusive B-Meson Decays","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"B. O. Lange, G. Paz (Cornell University), M. Neubert, S. W. Bosch","submitted_at":"2004-02-09T21:10:18Z","abstract_excerpt":"Using methods of effective field theory, factorized expressions for arbitrary B -> X_u l nu decay distributions in the shape-function region of large hadronic energy and moderate hadronic invariant mass are derived. Large logarithms are resummed at next-to-leading order in renormalization-group improved perturbation theory. The operator product expansion is employed to relate moments of the renormalized shape function with HQET parameters such as m_b, Lambda(bar) and lambda_1 defined in a new physical subtraction scheme. An analytic expression for the asymptotic behavior of the shape function "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0402094","kind":"arxiv","version":3},"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/0402094/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":"2026-07-04T16:48:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZkGwh3Og9sxV5yBbV7vbmGUKoRBkZVVQgAH2RXF59wQbV6mStffSfWZ/ygm0z7P0xWVRSdDzd3qq25gnrQeYCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-02T18:30:02.806207Z"},"content_sha256":"39c7e5fee3a438bc1be636b51ab56bb6b30d439c327d8c868d3af255e259e687","schema_version":"1.0","event_id":"sha256:39c7e5fee3a438bc1be636b51ab56bb6b30d439c327d8c868d3af255e259e687"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6XGCORNIJMMPLJY35CPC6D4ZTQ/bundle.json","state_url":"https://pith.science/pith/6XGCORNIJMMPLJY35CPC6D4ZTQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6XGCORNIJMMPLJY35CPC6D4ZTQ/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":"2026-08-02T18:30:02Z","links":{"resolver":"https://pith.science/pith/6XGCORNIJMMPLJY35CPC6D4ZTQ","bundle":"https://pith.science/pith/6XGCORNIJMMPLJY35CPC6D4ZTQ/bundle.json","state":"https://pith.science/pith/6XGCORNIJMMPLJY35CPC6D4ZTQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6XGCORNIJMMPLJY35CPC6D4ZTQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2004:6XGCORNIJMMPLJY35CPC6D4ZTQ","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":"de3aa6f27070024d37ec5dfb69a42f0d0112539cca602fd8e5fbb6d333ad1caf","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2004-02-09T21:10:18Z","title_canon_sha256":"88ca89469955f7b5aea6e20ac125521343ca271f44ebd950c089a6ed363d559f"},"schema_version":"1.0","source":{"id":"hep-ph/0402094","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0402094","created_at":"2026-07-04T16:48:06Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0402094v3","created_at":"2026-07-04T16:48:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0402094","created_at":"2026-07-04T16:48:06Z"},{"alias_kind":"pith_short_12","alias_value":"6XGCORNIJMMP","created_at":"2026-07-04T16:48:06Z"},{"alias_kind":"pith_short_16","alias_value":"6XGCORNIJMMPLJY3","created_at":"2026-07-04T16:48:06Z"},{"alias_kind":"pith_short_8","alias_value":"6XGCORNI","created_at":"2026-07-04T16:48:06Z"}],"graph_snapshots":[{"event_id":"sha256:39c7e5fee3a438bc1be636b51ab56bb6b30d439c327d8c868d3af255e259e687","target":"graph","created_at":"2026-07-04T16:48:06Z","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/0402094/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Using methods of effective field theory, factorized expressions for arbitrary B -> X_u l nu decay distributions in the shape-function region of large hadronic energy and moderate hadronic invariant mass are derived. Large logarithms are resummed at next-to-leading order in renormalization-group improved perturbation theory. The operator product expansion is employed to relate moments of the renormalized shape function with HQET parameters such as m_b, Lambda(bar) and lambda_1 defined in a new physical subtraction scheme. An analytic expression for the asymptotic behavior of the shape function ","authors_text":"B. O. Lange, G. Paz (Cornell University), M. Neubert, S. W. Bosch","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2004-02-09T21:10:18Z","title":"Factorization and Shape-Function Effects in Inclusive B-Meson Decays"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0402094","kind":"arxiv","version":3},"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":"sha256:224ae5630aa8ee7f325787fa4c013489df9cce3f04ff20e32dbb5b050d1b043b","target":"record","created_at":"2026-07-04T16:48:06Z","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":"de3aa6f27070024d37ec5dfb69a42f0d0112539cca602fd8e5fbb6d333ad1caf","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2004-02-09T21:10:18Z","title_canon_sha256":"88ca89469955f7b5aea6e20ac125521343ca271f44ebd950c089a6ed363d559f"},"schema_version":"1.0","source":{"id":"hep-ph/0402094","kind":"arxiv","version":3}},"canonical_sha256":"f5cc2745a84b18f5a71be89e2f0f999c3c266d193f87295522c50fd232d5aa81","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f5cc2745a84b18f5a71be89e2f0f999c3c266d193f87295522c50fd232d5aa81","first_computed_at":"2026-07-04T16:48:06.599574Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:48:06.599574Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"86YnIZtggADUWKreM1BtcDrHLQS4aAzsmZ56xgm0LFJvWs59UyggKXjSLaphqB/kgHr0KYVBVzYg80lQSUcNDg==","signature_status":"signed_v1","signed_at":"2026-07-04T16:48:06.599942Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0402094","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:224ae5630aa8ee7f325787fa4c013489df9cce3f04ff20e32dbb5b050d1b043b","sha256:39c7e5fee3a438bc1be636b51ab56bb6b30d439c327d8c868d3af255e259e687"],"state_sha256":"8bec806caba956d4fa780ae32d6ebe105b60b3fc7da371342006ae4b4801df29"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"F3HuFHXWT9GXJIEWHo5IAWXJfKM/FZfbPqGp0Re95twDeQwvV9Jmpp7M0bXWuJzwAku3MIrEzGKZxCmaC363AQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-02T18:30:02.811249Z","bundle_sha256":"92546d9b5d4e80f70c33dcbe9849753776eeeefabccbfadd5dc67c33df502057"}}