{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:4YFUA527U2VFCKWELBOP7BERUV","short_pith_number":"pith:4YFUA527","schema_version":"1.0","canonical_sha256":"e60b40775fa6aa512ac4585cff8491a57df14ecaacc006c4772a7ddd391e6224","source":{"kind":"arxiv","id":"1811.00983","version":2},"attestation_state":"computed","paper":{"title":"$B\\to P$ and $B\\to V$ Form Factors from $B$-Meson Light-Cone Sum Rules beyond Leading Twist","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Ahmet Kokulu, Danny van Dyk, Nico Gubernari","submitted_at":"2018-11-02T16:59:47Z","abstract_excerpt":"We provide results for the full set of form factors describing semileptonic $B$-meson transitions to pseudoscalar mesons $\\pi$, $K$, $\\bar{D}$ and vector mesons $\\rho$, $K^*$, $\\bar{D}^*$. Our results are obtained within the framework of QCD Light-Cone Sum Rules with $B$-meson distribution amplitudes. We recalculate and confirm the results for the leading-twist two-particle contributions in the literature. Furthermore, we calculate and provide new expressions for the two-particle contributions up to twist four. Following new developments for the three-particle distribution amplitudes, we calcu"},"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":"1811.00983","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-11-02T16:59:47Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"f97a7bc08bab647cf24a027d252bc14dcb64aeb9ee40a31b496b9476f4462ba8","abstract_canon_sha256":"6afd68f6dfc49622ce6eb83a03776d7d9ae17c94b9717ca938a0321d778b7bd8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:35:42.153307Z","signature_b64":"0IulesUI9JmT2eX2oOuhHSMHBzevqlrLQZStM1DOi/I2H3pTtnQ/8dBdmHNaygq7EiFyeVsyHAuUSPxDWf7IDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e60b40775fa6aa512ac4585cff8491a57df14ecaacc006c4772a7ddd391e6224","last_reissued_at":"2026-07-05T00:35:42.152826Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:35:42.152826Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$B\\to P$ and $B\\to V$ Form Factors from $B$-Meson Light-Cone Sum Rules beyond Leading Twist","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Ahmet Kokulu, Danny van Dyk, Nico Gubernari","submitted_at":"2018-11-02T16:59:47Z","abstract_excerpt":"We provide results for the full set of form factors describing semileptonic $B$-meson transitions to pseudoscalar mesons $\\pi$, $K$, $\\bar{D}$ and vector mesons $\\rho$, $K^*$, $\\bar{D}^*$. Our results are obtained within the framework of QCD Light-Cone Sum Rules with $B$-meson distribution amplitudes. We recalculate and confirm the results for the leading-twist two-particle contributions in the literature. Furthermore, we calculate and provide new expressions for the two-particle contributions up to twist four. Following new developments for the three-particle distribution amplitudes, we calcu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.00983","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/1811.00983/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":"1811.00983","created_at":"2026-07-05T00:35:42.152884+00:00"},{"alias_kind":"arxiv_version","alias_value":"1811.00983v2","created_at":"2026-07-05T00:35:42.152884+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1811.00983","created_at":"2026-07-05T00:35:42.152884+00:00"},{"alias_kind":"pith_short_12","alias_value":"4YFUA527U2VF","created_at":"2026-07-05T00:35:42.152884+00:00"},{"alias_kind":"pith_short_16","alias_value":"4YFUA527U2VFCKWE","created_at":"2026-07-05T00:35:42.152884+00:00"},{"alias_kind":"pith_short_8","alias_value":"4YFUA527","created_at":"2026-07-05T00:35:42.152884+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":10,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.21642","citing_title":"Probing Light Dark Fermions in $B \\to D^{(*)}\\ell X_{\\rm inv}$ via Rate Distributions","ref_index":53,"is_internal_anchor":false},{"citing_arxiv_id":"2607.01459","citing_title":"An introduction to Hammer v2: Helicity Amplitude Module for Matrix Element Reweighting","ref_index":61,"is_internal_anchor":false},{"citing_arxiv_id":"2606.17138","citing_title":"$|V_{cb}|$ determinations from $\\bar{B} \\to D^{(*)} \\ell \\bar\\nu$ decays within the SM and beyond","ref_index":11,"is_internal_anchor":false},{"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":33,"is_internal_anchor":false},{"citing_arxiv_id":"2606.07749","citing_title":"Flavor phenomenology of light dark particles","ref_index":241,"is_internal_anchor":false},{"citing_arxiv_id":"2605.26213","citing_title":"Unitarity bounds and form-factor predictions for $B$-meson decays","ref_index":96,"is_internal_anchor":false},{"citing_arxiv_id":"2604.26406","citing_title":"Semileptonic $B_q$ decays to heavy tensor mesons","ref_index":37,"is_internal_anchor":false},{"citing_arxiv_id":"2605.06567","citing_title":"Probing unknown nonperturbative effects in $b \\to s \\ell\\ell$ with inclusive and exclusive observables","ref_index":2,"is_internal_anchor":false},{"citing_arxiv_id":"2605.00181","citing_title":"Extracting production fractions of $b$ hadrons from exclusive semi-leptonic decays","ref_index":56,"is_internal_anchor":false},{"citing_arxiv_id":"2605.07997","citing_title":"Symmetry-Breaking Effects on Form Factors and Observables in $B \\to K_0^*(1430)\\mu^+\\mu^-$ Decay","ref_index":43,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4YFUA527U2VFCKWELBOP7BERUV","json":"https://pith.science/pith/4YFUA527U2VFCKWELBOP7BERUV.json","graph_json":"https://pith.science/api/pith-number/4YFUA527U2VFCKWELBOP7BERUV/graph.json","events_json":"https://pith.science/api/pith-number/4YFUA527U2VFCKWELBOP7BERUV/events.json","paper":"https://pith.science/paper/4YFUA527"},"agent_actions":{"view_html":"https://pith.science/pith/4YFUA527U2VFCKWELBOP7BERUV","download_json":"https://pith.science/pith/4YFUA527U2VFCKWELBOP7BERUV.json","view_paper":"https://pith.science/paper/4YFUA527","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1811.00983&json=true","fetch_graph":"https://pith.science/api/pith-number/4YFUA527U2VFCKWELBOP7BERUV/graph.json","fetch_events":"https://pith.science/api/pith-number/4YFUA527U2VFCKWELBOP7BERUV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4YFUA527U2VFCKWELBOP7BERUV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4YFUA527U2VFCKWELBOP7BERUV/action/storage_attestation","attest_author":"https://pith.science/pith/4YFUA527U2VFCKWELBOP7BERUV/action/author_attestation","sign_citation":"https://pith.science/pith/4YFUA527U2VFCKWELBOP7BERUV/action/citation_signature","submit_replication":"https://pith.science/pith/4YFUA527U2VFCKWELBOP7BERUV/action/replication_record"}},"created_at":"2026-07-05T00:35:42.152884+00:00","updated_at":"2026-07-05T00:35:42.152884+00:00"}