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In the on-shell renormalization scheme and for $\\alpha_s(m_b) \\cong 0.2$ we find a correction of -10% to the inclusive rate computed using factorization. This gives a total rate $BR(b \\to D_s^-(D^{*-}_s)c) \\cong 8%$ consistent within $1\\sigma$ with the measured value $BR(B \\to D_s^{\\pm}X) = (10.0 \\pm 2.5)%$. The general formulae give"},"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/9906505","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1999-06-25T16:33:21Z","cross_cats_sorted":[],"title_canon_sha256":"316258054a63de7468007f056760e04649e3fc65019c24ca87ea0f2c82a0b9e6","abstract_canon_sha256":"9c13c6dae172bc62980e42b4d9c1f6ab2419543a7bb0360434c1c90fce8e6eb4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:06:05.680480Z","signature_b64":"IcjCg7zKALK73SJyGcjYhr2FygP5ufF7kLfvGMYqARORC7grYsMBFG5/lWjW9sFsn9LxW/MaKVTrhCb4Nj7dDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f7b2c1d28027c5738519dcdde07cee3c78a71c98cb20ce54da3e5cb276e03060","last_reissued_at":"2026-05-18T01:06:05.679745Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:06:05.679745Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Inclusive decay of B mesons into $D_s$ or $D^*_s$","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Le Yaouanc, J.-C. Raynal, L. Oliver, M. Zito, O. Pene, R. Aleksan","submitted_at":"1999-06-25T16:33:21Z","abstract_excerpt":"We compute the inclusive decay rates $b \\to D_s^-(D^{*-}_s) c$ including lowest order QCD corrections on the quark legs, and compare with existing data. Unlike the short distance QCD corrections, that are of higher order, these corrections are of order $\\alpha_s$. In the on-shell renormalization scheme and for $\\alpha_s(m_b) \\cong 0.2$ we find a correction of -10% to the inclusive rate computed using factorization. This gives a total rate $BR(b \\to D_s^-(D^{*-}_s)c) \\cong 8%$ consistent within $1\\sigma$ with the measured value $BR(B \\to D_s^{\\pm}X) = (10.0 \\pm 2.5)%$. 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