{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:D4KHFMTBAAT2WABRXMLKH7KGMZ","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":"e3a26545c96e829370bdda4a3fbb611e2cd290961d0a3ab0ee66e16145516bf3","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-08-25T21:41:03Z","title_canon_sha256":"3cdfb5a3d9bb44f7827e86cd3b4551e11ba51b1be9763505a9075e139278eec7"},"schema_version":"1.0","source":{"id":"1908.09398","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1908.09398","created_at":"2026-07-05T00:41:35Z"},{"alias_kind":"arxiv_version","alias_value":"1908.09398v1","created_at":"2026-07-05T00:41:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1908.09398","created_at":"2026-07-05T00:41:35Z"},{"alias_kind":"pith_short_12","alias_value":"D4KHFMTBAAT2","created_at":"2026-07-05T00:41:35Z"},{"alias_kind":"pith_short_16","alias_value":"D4KHFMTBAAT2WABR","created_at":"2026-07-05T00:41:35Z"},{"alias_kind":"pith_short_8","alias_value":"D4KHFMTB","created_at":"2026-07-05T00:41:35Z"}],"graph_snapshots":[{"event_id":"sha256:23397b9073043f96c44ef90b7738222d0093f02af7c6aa579b2fe04a29f97bda","target":"graph","created_at":"2026-07-05T00:41:35Z","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/1908.09398/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We carry out an analysis of the full set of ten $\\bar{B}\\to D^{(*)}$ form factors within the framework of the Heavy-Quark Expansion (HQE) to order $\\mathcal{O}(\\alpha_s,\\,1/m_b,\\,1/m_c^2)$, both with and without the use of experimental data. This becomes possible due to a recent calculation of these form factors at and beyond the maximal physical recoil using QCD light-cone sum rules, in combination with constraints from lattice QCD, QCD three-point sum rules and unitarity. We find good agreement amongst the various theoretical results, as well as between the theoretical results and the kinema","authors_text":"Danny van Dyk, Martin Jung, Marzia Bordone","cross_cats":["hep-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1908.09398","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:d3878f93af806c4b984cc6ea9e9d610be53ce6483c2a61cf1bbdea84834fc9aa","target":"record","created_at":"2026-07-05T00:41:35Z","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":"e3a26545c96e829370bdda4a3fbb611e2cd290961d0a3ab0ee66e16145516bf3","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-08-25T21:41:03Z","title_canon_sha256":"3cdfb5a3d9bb44f7827e86cd3b4551e11ba51b1be9763505a9075e139278eec7"},"schema_version":"1.0","source":{"id":"1908.09398","kind":"arxiv","version":1}},"canonical_sha256":"1f1472b2610027ab0031bb16a3fd46666fe0427d5c84b746cc9217c062dc3338","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1f1472b2610027ab0031bb16a3fd46666fe0427d5c84b746cc9217c062dc3338","first_computed_at":"2026-07-05T00:41:35.985859Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T00:41:35.985859Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"qOCl350Vn69fo5eBKDSccRDwEafY2yO6Ztz3xUsfzT1XJr3lRN/K23CxW7cJ6FJKwLrA5PKntIBjtt7Dfy+3Bg==","signature_status":"signed_v1","signed_at":"2026-07-05T00:41:35.986346Z","signed_message":"canonical_sha256_bytes"},"source_id":"1908.09398","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d3878f93af806c4b984cc6ea9e9d610be53ce6483c2a61cf1bbdea84834fc9aa","sha256:23397b9073043f96c44ef90b7738222d0093f02af7c6aa579b2fe04a29f97bda"],"state_sha256":"ba85dd2566649c16ad05367ab4769e9ce5d26eafbdc8e136a4ad7da83da88985"}