{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1998:TYVBMCH5VP3P7TCSUKHCUV4OIE","short_pith_number":"pith:TYVBMCH5","canonical_record":{"source":{"id":"hep-ph/9809505","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1998-09-23T15:59:58Z","cross_cats_sorted":[],"title_canon_sha256":"e39be24a1836b51bfc52129adcce3d9fbaaeb225c5e2b2cdc43b7319413f38aa","abstract_canon_sha256":"b9109e7b5f2ed07998c2cec513222bd09dbffa1e9e57fa369af2408b21eea509"},"schema_version":"1.0"},"canonical_sha256":"9e2a1608fdabf6ffcc52a28e2a578e411932111de6bdc19869505558b7f8a8f3","source":{"kind":"arxiv","id":"hep-ph/9809505","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9809505","created_at":"2026-07-04T14:30:47Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9809505v1","created_at":"2026-07-04T14:30:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9809505","created_at":"2026-07-04T14:30:47Z"},{"alias_kind":"pith_short_12","alias_value":"TYVBMCH5VP3P","created_at":"2026-07-04T14:30:47Z"},{"alias_kind":"pith_short_16","alias_value":"TYVBMCH5VP3P7TCS","created_at":"2026-07-04T14:30:47Z"},{"alias_kind":"pith_short_8","alias_value":"TYVBMCH5","created_at":"2026-07-04T14:30:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1998:TYVBMCH5VP3P7TCSUKHCUV4OIE","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9809505","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1998-09-23T15:59:58Z","cross_cats_sorted":[],"title_canon_sha256":"e39be24a1836b51bfc52129adcce3d9fbaaeb225c5e2b2cdc43b7319413f38aa","abstract_canon_sha256":"b9109e7b5f2ed07998c2cec513222bd09dbffa1e9e57fa369af2408b21eea509"},"schema_version":"1.0"},"canonical_sha256":"9e2a1608fdabf6ffcc52a28e2a578e411932111de6bdc19869505558b7f8a8f3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:30:47.033823Z","signature_b64":"C6fz7yxJHiAxZ/NGkCpyJa/Yx2FpH0ymBmGClA9JAyLRrFo/MFoSsIycwd6o3E9xf7efP1kieUV944mClL9nAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9e2a1608fdabf6ffcc52a28e2a578e411932111de6bdc19869505558b7f8a8f3","last_reissued_at":"2026-07-04T14:30:47.033457Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:30:47.033457Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9809505","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":"2026-07-04T14:30:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3TTDdUTvD1C+gpuKu/D5kZME3TsgR/+bjjoYqdRWbTeDVPt4Zifb8oh+/Cx6o81SIL5Se1EhBwXhjiiP6S8pAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T19:58:36.664058Z"},"content_sha256":"6057bbe9e51f1888f640998cd2556993e0a2555bfe027efc7e506eb80c30eae9","schema_version":"1.0","event_id":"sha256:6057bbe9e51f1888f640998cd2556993e0a2555bfe027efc7e506eb80c30eae9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1998:TYVBMCH5VP3P7TCSUKHCUV4OIE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Improved QCD perturbative contributions and power corrections in radiative and semileptonic rare B decays","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Gudrun Hiller (DESY, Hamburg)","submitted_at":"1998-09-23T15:59:58Z","abstract_excerpt":"We calculate the leading power corrections to the decay rates, distributions and hadronic spectral moments in rare inclusive \\bxsll decays in the standard model, using heavy quark expansion (HQE) in $(1/m_b)$ and a phenomenological model implementing the Fermi motion effects of the b-quark bound in the B-hadron. We include next-to-leading order perturbative QCD corrections and work out the dependences of the spectra, decay rates and hadronic moments on the model parameters in either HQE and the Fermi motion model. In the latter, we take into account long-distance effects via $B \\to X_s +(J/\\ps"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9809505","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/9809505/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":"2026-07-04T14:30:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XfCbgvlUyBVu8Ei4RKt5yJWC3/URkY4SI39y0bLFq9bQYUEHaqx/bpyU6N9DkNpa3g3+rGtC7R9gi9YdwjdMCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T19:58:36.665028Z"},"content_sha256":"93c1de4a4141b483914dd96651f821ed5b950c83c305941af123ed2aab58a583","schema_version":"1.0","event_id":"sha256:93c1de4a4141b483914dd96651f821ed5b950c83c305941af123ed2aab58a583"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/TYVBMCH5VP3P7TCSUKHCUV4OIE/bundle.json","state_url":"https://pith.science/pith/TYVBMCH5VP3P7TCSUKHCUV4OIE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/TYVBMCH5VP3P7TCSUKHCUV4OIE/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":"2026-08-06T19:58:36Z","links":{"resolver":"https://pith.science/pith/TYVBMCH5VP3P7TCSUKHCUV4OIE","bundle":"https://pith.science/pith/TYVBMCH5VP3P7TCSUKHCUV4OIE/bundle.json","state":"https://pith.science/pith/TYVBMCH5VP3P7TCSUKHCUV4OIE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/TYVBMCH5VP3P7TCSUKHCUV4OIE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1998:TYVBMCH5VP3P7TCSUKHCUV4OIE","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":"b9109e7b5f2ed07998c2cec513222bd09dbffa1e9e57fa369af2408b21eea509","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1998-09-23T15:59:58Z","title_canon_sha256":"e39be24a1836b51bfc52129adcce3d9fbaaeb225c5e2b2cdc43b7319413f38aa"},"schema_version":"1.0","source":{"id":"hep-ph/9809505","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9809505","created_at":"2026-07-04T14:30:47Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9809505v1","created_at":"2026-07-04T14:30:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9809505","created_at":"2026-07-04T14:30:47Z"},{"alias_kind":"pith_short_12","alias_value":"TYVBMCH5VP3P","created_at":"2026-07-04T14:30:47Z"},{"alias_kind":"pith_short_16","alias_value":"TYVBMCH5VP3P7TCS","created_at":"2026-07-04T14:30:47Z"},{"alias_kind":"pith_short_8","alias_value":"TYVBMCH5","created_at":"2026-07-04T14:30:47Z"}],"graph_snapshots":[{"event_id":"sha256:93c1de4a4141b483914dd96651f821ed5b950c83c305941af123ed2aab58a583","target":"graph","created_at":"2026-07-04T14:30:47Z","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/9809505/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We calculate the leading power corrections to the decay rates, distributions and hadronic spectral moments in rare inclusive \\bxsll decays in the standard model, using heavy quark expansion (HQE) in $(1/m_b)$ and a phenomenological model implementing the Fermi motion effects of the b-quark bound in the B-hadron. We include next-to-leading order perturbative QCD corrections and work out the dependences of the spectra, decay rates and hadronic moments on the model parameters in either HQE and the Fermi motion model. In the latter, we take into account long-distance effects via $B \\to X_s +(J/\\ps","authors_text":"Gudrun Hiller (DESY, Hamburg)","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1998-09-23T15:59:58Z","title":"Improved QCD perturbative contributions and power corrections in radiative and semileptonic rare B decays"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9809505","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":"sha256:6057bbe9e51f1888f640998cd2556993e0a2555bfe027efc7e506eb80c30eae9","target":"record","created_at":"2026-07-04T14:30:47Z","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":"b9109e7b5f2ed07998c2cec513222bd09dbffa1e9e57fa369af2408b21eea509","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1998-09-23T15:59:58Z","title_canon_sha256":"e39be24a1836b51bfc52129adcce3d9fbaaeb225c5e2b2cdc43b7319413f38aa"},"schema_version":"1.0","source":{"id":"hep-ph/9809505","kind":"arxiv","version":1}},"canonical_sha256":"9e2a1608fdabf6ffcc52a28e2a578e411932111de6bdc19869505558b7f8a8f3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9e2a1608fdabf6ffcc52a28e2a578e411932111de6bdc19869505558b7f8a8f3","first_computed_at":"2026-07-04T14:30:47.033457Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T14:30:47.033457Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"C6fz7yxJHiAxZ/NGkCpyJa/Yx2FpH0ymBmGClA9JAyLRrFo/MFoSsIycwd6o3E9xf7efP1kieUV944mClL9nAg==","signature_status":"signed_v1","signed_at":"2026-07-04T14:30:47.033823Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9809505","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6057bbe9e51f1888f640998cd2556993e0a2555bfe027efc7e506eb80c30eae9","sha256:93c1de4a4141b483914dd96651f821ed5b950c83c305941af123ed2aab58a583"],"state_sha256":"9ef030ca85ecd13c083d096985cb0ed033e22491c1e1611504c9ad7461ffd232"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"npLywVZV6GBpGvYAHrRt1iXJKeiNdvGwvPrR7HFTAvZUqiCMaaaZ2wajfUOcGIEw8MHcbHHTQ+iRI5hrGlJvDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-06T19:58:36.671914Z","bundle_sha256":"ae4dac7441a1d39bfecadf132095cfe6f4a7439b3b67737622b1e19ef3cae0d9"}}