{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1994:6B575JGYH4AO24IF2BG6D3TCF3","short_pith_number":"pith:6B575JGY","schema_version":"1.0","canonical_sha256":"f07bfea4d83f00ed7105d04de1ee622edfa768b2119abc7afe5723e993b54339","source":{"kind":"arxiv","id":"hep-ph/9412229","version":1},"attestation_state":"computed","paper":{"title":"The $B \\to K^\\ast \\psi$ Polarization Puzzle","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Le Yaouanc, J.-C. Raynal, L. Oliver, O. P\\`ene, R. Aleksan","submitted_at":"1994-12-05T08:53:40Z","abstract_excerpt":"We point out that current estimates of form factors fail to explain the non-leptonic decays $B \\to \\psi K(K^{\\ast})$ and that the combination of data on the semi-leptonic decays $D \\to K(K^{\\ast})\\ell \\nu$ and on the non-leptonic decays $B \\to \\psi K(K^{\\ast})$ (in particular recent po\\-la\\-ri\\-za\\-tion data) severely constrain the form (normalization and $q^2$ dependence) of the heavy-to-light meson form factors, if we assume the factorization hypothesis for the latter. From a simultaneous fit to \\bpsi and \\dk data we find that strict heavy quark limit scaling laws applied to the form factors"},"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":"hep-ph/9412229","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1994-12-05T08:53:40Z","cross_cats_sorted":[],"title_canon_sha256":"074058ee1ada77651de3ac4761f713b9fcd6824f32f4a4f0ab109f8f272b37a5","abstract_canon_sha256":"1f837524c49d5b182296b91ac48cd702837546bdfbdecdda14f7c715ed6ff145"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:29:37.963817Z","signature_b64":"AngjF0b92oz6ZOyh9EnAnl6twlr/ijzjdP+ZGLImqo5sZMqe8jXrM+MbbY79VafzQCsyeL0QzyvGkdBWz6UIBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f07bfea4d83f00ed7105d04de1ee622edfa768b2119abc7afe5723e993b54339","last_reissued_at":"2026-07-04T14:29:37.963472Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:29:37.963472Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The $B \\to K^\\ast \\psi$ Polarization Puzzle","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Le Yaouanc, J.-C. Raynal, L. Oliver, O. P\\`ene, R. Aleksan","submitted_at":"1994-12-05T08:53:40Z","abstract_excerpt":"We point out that current estimates of form factors fail to explain the non-leptonic decays $B \\to \\psi K(K^{\\ast})$ and that the combination of data on the semi-leptonic decays $D \\to K(K^{\\ast})\\ell \\nu$ and on the non-leptonic decays $B \\to \\psi K(K^{\\ast})$ (in particular recent po\\-la\\-ri\\-za\\-tion data) severely constrain the form (normalization and $q^2$ dependence) of the heavy-to-light meson form factors, if we assume the factorization hypothesis for the latter. From a simultaneous fit to \\bpsi and \\dk data we find that strict heavy quark limit scaling laws applied to the form factors"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9412229","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/9412229/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":"hep-ph/9412229","created_at":"2026-07-04T14:29:37.963529+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9412229v1","created_at":"2026-07-04T14:29:37.963529+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9412229","created_at":"2026-07-04T14:29:37.963529+00:00"},{"alias_kind":"pith_short_12","alias_value":"6B575JGYH4AO","created_at":"2026-07-04T14:29:37.963529+00:00"},{"alias_kind":"pith_short_16","alias_value":"6B575JGYH4AO24IF","created_at":"2026-07-04T14:29:37.963529+00:00"},{"alias_kind":"pith_short_8","alias_value":"6B575JGY","created_at":"2026-07-04T14:29:37.963529+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6B575JGYH4AO24IF2BG6D3TCF3","json":"https://pith.science/pith/6B575JGYH4AO24IF2BG6D3TCF3.json","graph_json":"https://pith.science/api/pith-number/6B575JGYH4AO24IF2BG6D3TCF3/graph.json","events_json":"https://pith.science/api/pith-number/6B575JGYH4AO24IF2BG6D3TCF3/events.json","paper":"https://pith.science/paper/6B575JGY"},"agent_actions":{"view_html":"https://pith.science/pith/6B575JGYH4AO24IF2BG6D3TCF3","download_json":"https://pith.science/pith/6B575JGYH4AO24IF2BG6D3TCF3.json","view_paper":"https://pith.science/paper/6B575JGY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9412229&json=true","fetch_graph":"https://pith.science/api/pith-number/6B575JGYH4AO24IF2BG6D3TCF3/graph.json","fetch_events":"https://pith.science/api/pith-number/6B575JGYH4AO24IF2BG6D3TCF3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6B575JGYH4AO24IF2BG6D3TCF3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6B575JGYH4AO24IF2BG6D3TCF3/action/storage_attestation","attest_author":"https://pith.science/pith/6B575JGYH4AO24IF2BG6D3TCF3/action/author_attestation","sign_citation":"https://pith.science/pith/6B575JGYH4AO24IF2BG6D3TCF3/action/citation_signature","submit_replication":"https://pith.science/pith/6B575JGYH4AO24IF2BG6D3TCF3/action/replication_record"}},"created_at":"2026-07-04T14:29:37.963529+00:00","updated_at":"2026-07-04T14:29:37.963529+00:00"}