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With the vertex corrections and the NLO Wilson coefficients included, the branching ratios of the considered decays are $Br(B^+\\to J/\\Psi K_1(1270)^+)=1.76^{+0.65}_{-0.69}\\times10^{-3}, Br(B^+\\to J/\\Psi K_1(1400)^+)=7.03^{+2.70}_{-2.52}\\times10^{-4}$, and $Br(B^0\\to J/\\Psi K_1(1270)^0)=(1.63^{+0.60}_{-0.64})\\times10^{-3}$ with the mixing angle $\\theta_{K_1}=33^\\circ$, which can agree well with the data or the present experimental upper limit within errors. So we support the opinion that $\\"},"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":"1705.00524","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-05-01T14:03:04Z","cross_cats_sorted":[],"title_canon_sha256":"862b00cea0ce468c8f8bc7bf9d4703f63acca3927cea710e244567910f3b093e","abstract_canon_sha256":"65799ea7dd0d7feba9f2129f2d008e341fb24f85dbc1c0db720171bd6f9f4ddb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:48:06.940235Z","signature_b64":"MGpi5RvKjcUtpRASW7+htL+NqtT21cwvNqrQXt9K/t05Hz5vN3uQpo8nDGuhDHPKNjkI9NcyKH8GQz1ZzaIhAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"698dfeefd511aee6d177965c120917e971903c1ba026f180f6eb2ecea52a17af","last_reissued_at":"2026-05-17T23:48:06.939802Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:48:06.939802Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Study of the $K_1(1270)-K_1(1400)$ mixing in the decays $B\\to J/\\Psi K_1(1270), J/\\Psi K_1(1400)$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hongxia Guo, Si-Yang Wang, Zhi-Qing Zhang","submitted_at":"2017-05-01T14:03:04Z","abstract_excerpt":"We studied the B meson decays $B\\to J/\\Psi K_1(1270,1400)$ in the pQCD approach beyond the leading order. With the vertex corrections and the NLO Wilson coefficients included, the branching ratios of the considered decays are $Br(B^+\\to J/\\Psi K_1(1270)^+)=1.76^{+0.65}_{-0.69}\\times10^{-3}, Br(B^+\\to J/\\Psi K_1(1400)^+)=7.03^{+2.70}_{-2.52}\\times10^{-4}$, and $Br(B^0\\to J/\\Psi K_1(1270)^0)=(1.63^{+0.60}_{-0.64})\\times10^{-3}$ with the mixing angle $\\theta_{K_1}=33^\\circ$, which can agree well with the data or the present experimental upper limit within errors. 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