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Observation of B→D(*) π
Lees, J P; Poireau, V; Tisserand, V; Grauges, E; Palano, A; Eigen, G; Stugu, B; Brown, D N; Kerth, L T; Kolomensky, Yu G; Lee, M J; Lynch, G; Koch, H; Schroeder, T; Hearty, C; Mattison, T S; McKenna, J A; So, R Y; Khan, A; Blinov, V E; Buzykaev, A R; Druzhinin, V P; Golubev, V B; Kravchenko, E A; Onuchin, A P; Serednyakov, S I; Skovpen, Yu I; Solodov, E P; Todyshev, K Yu; Lankford, A J; Gary, J W; Long, O; Franco Sevilla, M; Hong, T M; Kovalskyi, D; Richman, J D; West, C A; Eisner, A M; Lockman, W S; Panduro Vazquez, W; Schumm, B A; Seiden, A; Chao, D S; Cheng, C H; Echenard, B; Flood, K T; Hitlin, D G; Kim, J; Miyashita, T S; Ongmongkolkul, P.
Affiliation
  • Lees JP; Laboratoire d'Annecy-le-Vieux de Physique des Particules (LAPP), Université de Savoie, CNRS/IN2P3, F-74941 Annecy-Le-Vieux, France.
  • Poireau V; Laboratoire d'Annecy-le-Vieux de Physique des Particules (LAPP), Université de Savoie, CNRS/IN2P3, F-74941 Annecy-Le-Vieux, France.
  • Tisserand V; Laboratoire d'Annecy-le-Vieux de Physique des Particules (LAPP), Université de Savoie, CNRS/IN2P3, F-74941 Annecy-Le-Vieux, France.
  • Grauges E; Facultat de Fisica, Departament ECM, Universitat de Barcelona, E-08028 Barcelona, Spain.
  • Palano A; INFN Sezione di Bari, I-70126 Bari, Italy.
  • Eigen G; Dipartimento di Fisica, Università di Bari, I-70126 Bari, Italy.
  • Stugu B; Institute of Physics, University of Bergen, N-5007 Bergen, Norway.
  • Brown DN; Institute of Physics, University of Bergen, N-5007 Bergen, Norway.
  • Kerth LT; Lawrence Berkeley National Laboratory and University of California, Berkeley, California 94720, USA.
  • Kolomensky YG; Lawrence Berkeley National Laboratory and University of California, Berkeley, California 94720, USA.
  • Lee MJ; Lawrence Berkeley National Laboratory and University of California, Berkeley, California 94720, USA.
  • Lynch G; Lawrence Berkeley National Laboratory and University of California, Berkeley, California 94720, USA.
  • Koch H; Lawrence Berkeley National Laboratory and University of California, Berkeley, California 94720, USA.
  • Schroeder T; Institut für Experimentalphysik 1, Ruhr Universität Bochum, D-44780 Bochum, Germany.
  • Hearty C; Institut für Experimentalphysik 1, Ruhr Universität Bochum, D-44780 Bochum, Germany.
  • Mattison TS; University of British Columbia, Vancouver, British Columbia V6T 1Z1, Canada.
  • McKenna JA; University of British Columbia, Vancouver, British Columbia V6T 1Z1, Canada.
  • So RY; University of British Columbia, Vancouver, British Columbia V6T 1Z1, Canada.
  • Khan A; University of British Columbia, Vancouver, British Columbia V6T 1Z1, Canada.
  • Blinov VE; Brunel University, Uxbridge, Middlesex UB8 3PH, United Kingdom.
  • Buzykaev AR; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Druzhinin VP; Novosibirsk State University, Novosibirsk 630090, Russia.
  • Golubev VB; Novosibirsk State Technical University, Novosibirsk 630092, Russia.
  • Kravchenko EA; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Onuchin AP; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Serednyakov SI; Novosibirsk State University, Novosibirsk 630090, Russia.
  • Skovpen YI; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Solodov EP; Novosibirsk State University, Novosibirsk 630090, Russia.
  • Todyshev KY; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Lankford AJ; Novosibirsk State University, Novosibirsk 630090, Russia.
  • Gary JW; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Long O; Novosibirsk State University, Novosibirsk 630090, Russia.
  • Franco Sevilla M; Novosibirsk State Technical University, Novosibirsk 630092, Russia.
  • Hong TM; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Kovalskyi D; Novosibirsk State University, Novosibirsk 630090, Russia.
  • Richman JD; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • West CA; Novosibirsk State University, Novosibirsk 630090, Russia.
  • Eisner AM; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Lockman WS; Novosibirsk State University, Novosibirsk 630090, Russia.
  • Panduro Vazquez W; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Schumm BA; Novosibirsk State University, Novosibirsk 630090, Russia.
  • Seiden A; University of California at Irvine, Irvine, California 92697, USA.
  • Chao DS; University of California at Riverside, Riverside, California 92521, USA.
  • Cheng CH; University of California at Riverside, Riverside, California 92521, USA.
  • Echenard B; University of California at Santa Barbara, Santa Barbara, California 93106, USA.
  • Flood KT; University of California at Santa Barbara, Santa Barbara, California 93106, USA.
  • Hitlin DG; University of California at Santa Barbara, Santa Barbara, California 93106, USA.
  • Kim J; University of California at Santa Barbara, Santa Barbara, California 93106, USA.
  • Miyashita TS; University of California at Santa Barbara, Santa Barbara, California 93106, USA.
  • Ongmongkolkul P; Institute for Particle Physics, University of California at Santa Cruz, Santa Cruz, California 95064, USA.
Phys Rev Lett ; 116(4): 041801, 2016 Jan 29.
Article in En | MEDLINE | ID: mdl-26871322
ABSTRACT
We report on measurements of the decays of B¯ mesons into the semileptonic final states B¯â†’D^(*)π^(+)π^(-)ℓ^(-)ν¯, where D^(*) represents a D or D^(*) meson and ℓ^(-) is an electron or a muon. These measurements are based on 471×10^(6) BB ¯ pairs recorded with the BABAR detector at the SLAC asymmetric B factory PEP-II. We determine the branching fraction ratios R_{π^{+}π^{-}}^{(*)}=B(B[over ¯]→D^{(*)}π^{+}π^{-}ℓ^{-}ν[over ¯])/B(B[over ¯]→D^{(*)}ℓ^{-}ν[over ¯]) using events in which the second B meson is fully reconstructed. We find R_{π^{+}π^{-}}=0.067±0.010±0.008 and R_{π^{+}π^{-}}^{*}=0.019±0.005±0.004, where the first uncertainty is statistical and the second is systematic. Based on these results and assuming isospin invariance, we estimate that B[over ¯]→D^{(*)}ππℓ^{-}ν[over ¯] decays, where π denotes either a π^{±} and π^{0} meson, account for up to half the difference between the measured inclusive semileptonic branching fraction to charm hadrons and the corresponding sum of previously measured exclusive branching fractions.

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Phys Rev Lett Year: 2016 Document type: Article Affiliation country:

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Phys Rev Lett Year: 2016 Document type: Article Affiliation country: