{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2008:FFFRGDF27EJXLUBHPNGACCQU5N","short_pith_number":"pith:FFFRGDF2","schema_version":"1.0","canonical_sha256":"294b130cbaf91375d0277b4c010a14eb7daf24c63940d43be0d5e72e0a160beb","source":{"kind":"arxiv","id":"0803.3561","version":2},"attestation_state":"computed","paper":{"title":"Complete Michel Parameter Analysis of inclusive semileptonic b \\to c transition","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Benjamin Dassinger, Robert Feger, Thomas Mannel","submitted_at":"2008-03-25T13:42:35Z","abstract_excerpt":"We perform a complete \"Michel parameter\" analysis of all possible helicity structures which can appear in the process $B \\to X_c \\ell \\bar{\\nu}_\\ell$. We take into account the full set of operators parametrizing the effective Hamiltonian and include the complete one-loop QCD corrections as well as the non-perturbative contributions. The moments of the leptonic energy as well as the combined moments of the hadronic energy and hadronic invariant mass are calculated including the non-standard contributions."},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"0803.3561","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2008-03-25T13:42:35Z","cross_cats_sorted":[],"title_canon_sha256":"97770ed15b5ae43be645157719a05e29fac9ca711e0a3918345bbd815b6f4db7","abstract_canon_sha256":"e420751a7cccfb3ba58c570d5e3a69f91472226e1c310f167cf63eeb2c944ad4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:21:58.129711Z","signature_b64":"YvkSBhzbHoc0Axe4JELo6ZnQ5H2f6bNaSQp/+e1tos5N3KatnB3AA9CQKZ7sBIMP2TPst7+uWBjWJ/DHOzuxCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"294b130cbaf91375d0277b4c010a14eb7daf24c63940d43be0d5e72e0a160beb","last_reissued_at":"2026-07-04T16:21:58.129367Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:21:58.129367Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Complete Michel Parameter Analysis of inclusive semileptonic b \\to c transition","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Benjamin Dassinger, Robert Feger, Thomas Mannel","submitted_at":"2008-03-25T13:42:35Z","abstract_excerpt":"We perform a complete \"Michel parameter\" analysis of all possible helicity structures which can appear in the process $B \\to X_c \\ell \\bar{\\nu}_\\ell$. We take into account the full set of operators parametrizing the effective Hamiltonian and include the complete one-loop QCD corrections as well as the non-perturbative contributions. The moments of the leptonic energy as well as the combined moments of the hadronic energy and hadronic invariant mass are calculated including the non-standard contributions."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0803.3561","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/0803.3561/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"0803.3561","created_at":"2026-07-04T16:21:58.129424+00:00"},{"alias_kind":"arxiv_version","alias_value":"0803.3561v2","created_at":"2026-07-04T16:21:58.129424+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0803.3561","created_at":"2026-07-04T16:21:58.129424+00:00"},{"alias_kind":"pith_short_12","alias_value":"FFFRGDF27EJX","created_at":"2026-07-04T16:21:58.129424+00:00"},{"alias_kind":"pith_short_16","alias_value":"FFFRGDF27EJXLUBH","created_at":"2026-07-04T16:21:58.129424+00:00"},{"alias_kind":"pith_short_8","alias_value":"FFFRGDF2","created_at":"2026-07-04T16:21:58.129424+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.02276","citing_title":"A Comprehensive Analysis of $B_s \\to D_s^{**}\\ell\\nu_\\ell$ Decays Within and Beyond the Standard Model","ref_index":21,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FFFRGDF27EJXLUBHPNGACCQU5N","json":"https://pith.science/pith/FFFRGDF27EJXLUBHPNGACCQU5N.json","graph_json":"https://pith.science/api/pith-number/FFFRGDF27EJXLUBHPNGACCQU5N/graph.json","events_json":"https://pith.science/api/pith-number/FFFRGDF27EJXLUBHPNGACCQU5N/events.json","paper":"https://pith.science/paper/FFFRGDF2"},"agent_actions":{"view_html":"https://pith.science/pith/FFFRGDF27EJXLUBHPNGACCQU5N","download_json":"https://pith.science/pith/FFFRGDF27EJXLUBHPNGACCQU5N.json","view_paper":"https://pith.science/paper/FFFRGDF2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0803.3561&json=true","fetch_graph":"https://pith.science/api/pith-number/FFFRGDF27EJXLUBHPNGACCQU5N/graph.json","fetch_events":"https://pith.science/api/pith-number/FFFRGDF27EJXLUBHPNGACCQU5N/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FFFRGDF27EJXLUBHPNGACCQU5N/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FFFRGDF27EJXLUBHPNGACCQU5N/action/storage_attestation","attest_author":"https://pith.science/pith/FFFRGDF27EJXLUBHPNGACCQU5N/action/author_attestation","sign_citation":"https://pith.science/pith/FFFRGDF27EJXLUBHPNGACCQU5N/action/citation_signature","submit_replication":"https://pith.science/pith/FFFRGDF27EJXLUBHPNGACCQU5N/action/replication_record"}},"created_at":"2026-07-04T16:21:58.129424+00:00","updated_at":"2026-07-04T16:21:58.129424+00:00"}