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Improved measurement of the absolute branching fraction of D⁺rightarrow bar K⁰ μ⁺ν_(μ)

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arxiv 1605.00068 v2 pith:6GUPLKYQ submitted 2016-04-30 hep-ex

Improved measurement of the absolute branching fraction of D⁺rightarrow bar K⁰ μ⁺ν_(μ)

M.Ablikim , M.N.Achasov , X.C.Ai , O.Albayrak , M.Albrecht , D.J.Ambrose , A.Amoroso , F.F.An
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Q.An J.Z.Bai R.Baldini Ferroli Y.Ban D.W.Bennett J.V.Bennett M.Bertani D.Bettoni J.M.Bian F.Bianchi E.Boger I.Boyko R.A.Briere H.Cai X.Cai O. Cakir A.Calcaterra G.F.Cao S.A.Cetin J.F.Chang G.Chelkov G.Chen H.S.Chen H.Y.Chen J.C.Chen M.L.Chen S.Chen S.J.Chen X.Chen X.R.Chen Y.B.Chen H.P.Cheng X.K.Chu G.Cibinetto H.L.Dai J.P.Dai A.Dbeyssi D.Dedovich Z.Y.Deng A.Denig I.Denysenko M.Destefanis F.DeMori Y.Ding C.Dong J.Dong L.Y.Dong M.Y.Dong Z.L.Dou S.X.Du P.F.Duan J.Z.Fan J.Fang S.S.Fang X.Fang Y.Fang R.Farinelli L.Fava O.Fedorov F.Feldbauer G.Felici C.Q.Feng E.Fioravanti M. Fritsch C.D.Fu Q.Gao X.L.Gao X.Y.Gao Y.Gao Z.Gao I.Garzia K.Goetzen L.Gong W.X.Gong W.Gradl M.Greco M.H.Gu Y.T.Gu Y.H.Guan A.Q.Guo L.B.Guo R.P.Guo Y.Guo Y.P.Guo Z.Haddadi A.Hafner S.Han X.Q.Hao F.A.Harris K.L.He T.Held Y.K.Heng Z.L.Hou C.Hu H.M.Hu J.F.Hu T.Hu Y.Hu G.S.Huang J.S.Huang X.T.Huang X.Z.Huang Y.Huang Z.L.Huang T.Hussain Q.Ji Q.P.Ji X.B.Ji X.L.Ji L.W.Jiang X.S.Jiang X.Y.Jiang J.B.Jiao Z.Jiao D.P.Jin S.Jin T.Johansson A.Julin N.Kalantar-Nayestanaki X.L.Kang X.S.Kang M.Kavatsyuk B.C.Ke P. Kiese R.Kliemt B.Kloss O.B.Kolcu B.Kopf M.Kornicer A.Kupsc W.K\"uhn J.S.Lange M.Lara P. Larin C.Leng C.Li Cheng Li D.M.Li F.Li F.Y.Li G.Li H.B.Li H.J.Li J.C.LI Jin Li K.Li Lei Li P.R.Li Q.Y.Li T. Li W.D.Li W.G.Li X.L.Li X.N.Li X.Q.Li Y.B.Li Z.B.Li H.Liang Y.F.Liang Y.T.Liang G.R.Liao D.X.Lin B.Liu B.J.Liu C.X.Liu D.Liu F.H.Liu Fang Liu Feng Liu H.B.Liu H.H.Liu H.M.Liu J.Liu J.B.Liu J.P.Liu J.Y.Liu K.Liu K.Y.Liu L.D.Liu P.L.Liu Q.Liu S.B.Liu X.Liu Y.B.Liu Z.A.Liu Zhiqing Liu H.Loehner X.C.Lou H.J.Lu J.G.Lu Y.LU Y.P.Lu C.L.Luo M.X.Luo T.Luo X.L.Luo X.R.Lyu F.C.Ma H.L.Ma L.L. Ma M.M.Ma Q.M.Ma T.Ma X.N.Ma X.Y.Ma Y.M.Ma F.E.Maas M.Maggiora Y.J.Mao Z.P.Mao S.Marcello J.G.Messchendorp J.Min T.J.Min R.E.Mitchell X.H.Mo Y.J.Mo C.Morales Morales N.Yu.Muchnoi H.Muramatsu Y.Nefedov F.Nerling I.B.Nikolaev Z.Ning S.Nisar S.L.Niu X.Y.Niu S.L.Olsen Q.Ouyang S.Pacetti Y.Pan P.Patteri M.Pelizaeus H.P.Peng K.Peters J.Pettersson J.L.Ping R.G.Ping R.Poling V.Prasad H.R.Qi M.Qi S.Qian C.F.Qiao L.Q.Qin N.Qin X.S.Qin Z.H.Qin J.F.Qiu K.H.Rashid C.F.Redmer M.Ripka G.Rong Ch.Rosner X.D.Ruan A.Sarantsev M.Savri\'e K.Schoenning S.Schumann W.Shan M.Shao C.P.Shen P.X.Shen X.Y.Shen H.Y.Sheng M.Shi W.M.Song X.Y.Song S.Sosio S.Spataro G.X.Sun J.F.Sun S.S.Sun X.H.Sun Y.J.Sun Y.Z.Sun Z.J.Sun Z.T.Sun C.J.Tang X.Tang I.Tapan E.H.Thorndike M.Tiemens M.Ullrich I.Uman G.S.Varner B.Wang B.L.Wang D.Wang D.Y.Wang K.Wang L.L.Wang L.S.Wang M.Wang P.Wang P.L.Wang W.Wang W.P.Wang X.F. Wang Y.Wang Y.D.Wang Y.F.Wang Y.Q.Wang Z.Wang Z.G.Wang Z.H.Wang Z.Y.Wang T.Weber D.H.Wei P.Weidenkaff S.P.Wen U.Wiedner M.Wolke L.H.Wu L.J.Wu Z.Wu L.Xia L.G.Xia Y.Xia D.Xiao H.Xiao Z.J.Xiao Y.G.Xie Q.L.Xiu G.F.Xu J.J.Xu L.Xu Q.J.Xu Q.N.Xu X.P.Xu L.Yan W.B.Yan W.C.Yan Y.H.Yan H.J.Yang H.X.Yang L.Yang Y.X.Yang M.Ye M.H.Ye J.H.Yin B.X.Yu C.X.Yu J.S.Yu C.Z.Yuan W.L.Yuan Y.Yuan A.Yuncu A.A.Zafar A.Zallo Y.Zeng Z.Zeng B.X.Zhang B.Y.Zhang C.Zhang C.C.Zhang D.H.Zhang H.H.Zhang H.Y.Zhang J.Zhang J.J.Zhang J.L.Zhang J.Q.Zhang J.W.Zhang J.Y.Zhang J.Z.Zhang K.Zhang L.Zhang S.Q.Zhang X.Y.Zhang Y.Zhang Y.H.Zhang Y.N.Zhang Y.T.Zhang Yu Zhang Z.H.Zhang Z.P.Zhang Z.Y.Zhang G.Zhao J.W.Zhao J.Y.Zhao J.Z.Zhao Lei Zhao Ling Zhao M.G.Zhao Q.Zhao Q.W.Zhao S.J.Zhao T.C.Zhao Y.B.Zhao Z.G.Zhao A.Zhemchugov B.Zheng J.P.Zheng W.J.Zheng Y.H.Zheng B.Zhong L.Zhou X.Zhou X.K.Zhou X.R.Zhou X.Y.Zhou K.Zhu K.J.Zhu S.Zhu S.H.Zhu X.L.Zhu Y.C.Zhu Y.S.Zhu Z.A.Zhu J.Zhuang L.Zotti B.S.Zou J.H.Zou
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keywords rightarrowgammamathcalabsolutebranchingdatafractionimproved
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By analyzing 2.93 fb$^{-1}$ of data collected at $\sqrt s=3.773$ GeV with the BESIII detector, we measure the absolute branching fraction ${\mathcal B}(D^{+}\rightarrow\bar K^0\mu^{+}\nu_{\mu})=(8.72 \pm 0.07_{\rm stat.} \pm 0.18_{\rm sys.})\%$, which is consistent with previous measurements within uncertainties but with significantly improved precision. Combining the Particle Data Group values of ${\mathcal B}(D^0\to K^-\mu^+\nu_\mu)$, ${\mathcal B}(D^{+}\rightarrow\bar K^0 e^{+}\nu_{e})$, and the lifetimes of the $D^0$ and $D^+$ mesons with the value of ${\mathcal B}(D^{+}\rightarrow\bar K^0 \mu^{+}\nu_{\mu})$ measured in this work, we determine the following ratios of partial widths: $\Gamma(D^0\to K^-\mu^+\nu_\mu)/\Gamma(D^{+}\rightarrow\bar K^0\mu^{+}\nu_{\mu})=0.963\pm0.044$ and $\Gamma(D^{+}\rightarrow\bar K^0 \mu^{+}\nu_{\mu})/\Gamma(D^{+}\rightarrow\bar K^0 e^{+}\nu_{e})=0.988\pm0.033$.

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