Abstract
We report a measurement of the branching fractions of the decays B→D(∗)πν. The analysis uses 772×106 BB. pairs produced in e+e-→(4S) data recorded by the Belle experiment at the KEKB asymmetric-energy e+e- collider. The tagging B meson in the decay is fully reconstructed in a hadronic decay mode. On the signal side, we reconstruct the decay B→D(∗)πν(=e,μ). The measured branching fractions are B(B+→D-π++ν)=[4.55±0.27 (stat.)±0.39 (syst.)]×10-3, B(B0→D.0π-+ν)=[4.05±0.36 (stat.)±0.41 (syst.)]×10-3, B(B+→D∗-π++ν)=[6.03±0.43 (stat.)±0.38 (syst.)]×10-3, and B(B0→D.∗0π-+ν)=[6.46±0.53 (stat.)±0.52 (syst.)]×10-3. These are in good agreement with the current world-average values.
Original language | English |
---|---|
Article number | 012005 |
Journal | Physical Review D |
Volume | 98 |
Issue number | 1 |
DOIs | |
Publication status | Published - 2018 Jul 1 |
ASJC Scopus subject areas
- Nuclear and High Energy Physics
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In: Physical Review D, Vol. 98, No. 1, 012005, 01.07.2018.
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TY - JOUR
T1 - Measurement of the branching fraction of B →d (∗)πν at Belle using hadronic tagging in fully reconstructed events
AU - Vossen, A.
AU - Adachi, I.
AU - Adamczyk, K.
AU - Aihara, H.
AU - Al Said, S.
AU - Asner, D. M.
AU - Aulchenko, V.
AU - Aushev, T.
AU - Ayad, R.
AU - Badhrees, I.
AU - Bansal, V.
AU - Beleño, C.
AU - Bhuyan, B.
AU - Bilka, T.
AU - Biswal, J.
AU - Bondar, A.
AU - Bozek, A.
AU - Browder, T. E.
AU - Červenkov, D.
AU - Chen, A.
AU - Cheon, B. G.
AU - Chilikin, K.
AU - Cho, K.
AU - Choi, S. K.
AU - Choi, Y.
AU - Choudhury, S.
AU - Cinabro, D.
AU - Cunliffe, S.
AU - Dash, N.
AU - Di Carlo, S.
AU - DoleŽal, Z.
AU - Eidelman, S.
AU - Fast, J. E.
AU - Ferber, T.
AU - Fulsom, B. G.
AU - Garg, R.
AU - Gaur, V.
AU - Gabyshev, N.
AU - Garmash, A.
AU - Gelb, M.
AU - Goldenzweig, P.
AU - Guido, E.
AU - Hara, T.
AU - Hartbrich, O.
AU - Hayasaka, K.
AU - Hayashii, H.
AU - Hedges, M. T.
AU - Hirose, S.
AU - Hou, W. S.
AU - Inami, K.
AU - Ishikawa, A.
AU - Itoh, R.
AU - Iwasaki, M.
AU - Iwasaki, Y.
AU - Jacobs, W. W.
AU - Jaegle, I.
AU - Jia, S.
AU - Jin, Y.
AU - Julius, T.
AU - Kim, D. Y.
AU - Kim, H. J.
AU - Kim, J. B.
AU - Kim, K. T.
AU - Kim, S. H.
AU - Kinoshita, K.
AU - Korpar, S.
AU - Kotchetkov, D.
AU - KriŽan, P.
AU - Kroeger, R.
AU - Krokovny, P.
AU - Kuhr, T.
AU - Kulasiri, R.
AU - Kumita, T.
AU - Kwon, Y. J.
AU - Lange, J. S.
AU - Lee, I. S.
AU - Lee, S. C.
AU - Li, L. K.
AU - Li, Y.
AU - Li Gioi, L.
AU - Libby, J.
AU - Liventsev, D.
AU - Lubej, M.
AU - Masuda, M.
AU - Merola, M.
AU - Miyabayashi, K.
AU - Miyata, H.
AU - Mizuk, R.
AU - Moon, H. K.
AU - Mussa, R.
AU - Nakano, E.
AU - Nakao, M.
AU - Nanut, T.
AU - Nath, K. J.
AU - Nayak, M.
AU - Niiyama, M.
AU - Nishida, S.
AU - Ono, H.
AU - Pakhlov, P.
AU - Pakhlova, G.
AU - Pal, B.
AU - Pardi, S.
AU - Park, H.
AU - Paul, S.
AU - Pedlar, T. K.
AU - Pestotnik, R.
AU - Piilonen, L. E.
AU - Popov, V.
AU - Ritter, M.
AU - Rostomyan, A.
AU - Russo, G.
AU - Sahoo, D.
AU - Sakai, Y.
AU - Salehi, M.
AU - Sandilya, S.
AU - Santelj, L.
AU - Sanuki, T.
AU - Savinov, V.
AU - Schneider, O.
AU - Schnell, G.
AU - Schwanda, C.
AU - Schwartz, A. J.
AU - Seino, Y.
AU - Senyo, K.
AU - Shebalin, V.
AU - Shen, C. P.
AU - Shibata, T. A.
AU - Shimizu, N.
AU - Shiu, J. G.
AU - Simon, F.
AU - Solovieva, E.
AU - Starič, M.
AU - Strube, J. F.
AU - Sumihama, M.
AU - Sumiyoshi, T.
AU - Takizawa, M.
AU - Tamponi, U.
AU - Tanida, K.
AU - Tenchini, F.
AU - Trabelsi, K.
AU - Uchida, M.
AU - Uglov, T.
AU - Unno, Y.
AU - Uno, S.
AU - Urquijo, P.
AU - Usov, Y.
AU - Van Hulse, C.
AU - Varner, G.
AU - Varvell, K. E.
AU - Vinokurova, A.
AU - Vorobyev, V.
AU - Wang, B.
AU - Wang, C. H.
AU - Wang, M. Z.
AU - Wang, P.
AU - Watanabe, M.
AU - Widmann, E.
AU - Won, E.
AU - Ye, H.
AU - Yusa, Y.
AU - Zakharov, S.
AU - Zhang, Z. P.
AU - Zhilich, V.
AU - Zhukova, V.
AU - Zhulanov, V.
AU - Zupanc, A.
N1 - Funding Information: We thank the KEKB group for the excellent operation of the accelerator; the KEK cryogenics group for the efficient operation of the solenoid; and the KEK computer group, the National Institute of Informatics, and the Pacific Northwest National Laboratory (PNNL) Environmental Molecular Sciences Laboratory (EMSL) computing group for valuable computing and Science Information NETwork 5 (SINET5) network support. We acknowledge support from the Ministry of Education, Culture, Sports, Science, and Technology (MEXT) of Japan, the Japan Society for the Promotion of Science (JSPS), and the Tau-Lepton Physics Research Center of Nagoya University; the Australian Research Council; Austrian Science Fund under Grant No. P 26794-N20; the National Natural Science Foundation of China under Contracts No. 11435013, No. 11475187, No. 11521505, No. 11575017, No. 11675166, and No. 11705209; Key Research Program of Frontier Sciences, Chinese Academy of Sciences (CAS), Grant No. QYZDJ-SSW-SLH011; the CAS Center for Excellence in Particle Physics (CCEPP); Fudan University Grants No. JIH5913023, No. IDH5913011/003, No. JIH5913024, and No. IDH5913011/002; the Ministry of Education, Youth and Sports of the Czech Republic under Contract No. LTT17020; the Carl Zeiss Foundation, the Deutsche Forschungsgemeinschaft, the Excellence Cluster Universe, and the VolkswagenStiftung; the Department of Science and Technology of India; the Istituto Nazionale di Fisica Nucleare of Italy; National Research Foundation (NRF) of Korea Grants No. 2014R1A2A2A01005286, No. 2015R1A2A2A01003280, No. 2015H1A2A1033649, No. 2016R1D1A1B01010135, No. 2016K1A3A7A09005 603, and No. 2016R1D1A1B02012900; Radiation Science Research Institute, Foreign Large-Size Research Facility Application Supporting project and the Global Science Experimental Data Hub Center of the Korea Institute of Science and Technology Information; the Polish Ministry of Science and Higher Education and the National Science Center; the Ministry of Education and Science of the Russian Federation and the Russian Foundation for Basic Research; the Slovenian Research Agency; Ikerbasque, Basque Foundation for Science, Basque Government (No. IT956-16) and Ministry of Economy and Competitiveness (MINECO) (Juan de la Cierva), Spain; the Swiss National Science Foundation; the Ministry of Education and the Ministry of Science and Technology of Taiwan; and the United States Department of Energy and the National Science Foundation. Publisher Copyright: © 2018 authors. Published by the American Physical Society.
PY - 2018/7/1
Y1 - 2018/7/1
N2 - We report a measurement of the branching fractions of the decays B→D(∗)πν. The analysis uses 772×106 BB. pairs produced in e+e-→(4S) data recorded by the Belle experiment at the KEKB asymmetric-energy e+e- collider. The tagging B meson in the decay is fully reconstructed in a hadronic decay mode. On the signal side, we reconstruct the decay B→D(∗)πν(=e,μ). The measured branching fractions are B(B+→D-π++ν)=[4.55±0.27 (stat.)±0.39 (syst.)]×10-3, B(B0→D.0π-+ν)=[4.05±0.36 (stat.)±0.41 (syst.)]×10-3, B(B+→D∗-π++ν)=[6.03±0.43 (stat.)±0.38 (syst.)]×10-3, and B(B0→D.∗0π-+ν)=[6.46±0.53 (stat.)±0.52 (syst.)]×10-3. These are in good agreement with the current world-average values.
AB - We report a measurement of the branching fractions of the decays B→D(∗)πν. The analysis uses 772×106 BB. pairs produced in e+e-→(4S) data recorded by the Belle experiment at the KEKB asymmetric-energy e+e- collider. The tagging B meson in the decay is fully reconstructed in a hadronic decay mode. On the signal side, we reconstruct the decay B→D(∗)πν(=e,μ). The measured branching fractions are B(B+→D-π++ν)=[4.55±0.27 (stat.)±0.39 (syst.)]×10-3, B(B0→D.0π-+ν)=[4.05±0.36 (stat.)±0.41 (syst.)]×10-3, B(B+→D∗-π++ν)=[6.03±0.43 (stat.)±0.38 (syst.)]×10-3, and B(B0→D.∗0π-+ν)=[6.46±0.53 (stat.)±0.52 (syst.)]×10-3. These are in good agreement with the current world-average values.
UR - http://www.scopus.com/inward/record.url?scp=85051029727&partnerID=8YFLogxK
U2 - 10.1103/PhysRevD.98.012005
DO - 10.1103/PhysRevD.98.012005
M3 - Article
AN - SCOPUS:85051029727
SN - 2470-0010
VL - 98
JO - Physical Review D
JF - Physical Review D
IS - 1
M1 - 012005
ER -