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Extraction of form Factors from a Four-Dimensional Angular Analysis of B[over ¯]→D
Lees, J P; Poireau, V; Tisserand, V; Grauges, E; Palano, A; Eigen, G; Brown, D N; Kolomensky, Yu G; Fritsch, M; Koch, H; Schroeder, T; Hearty, C; Mattison, T S; McKenna, J A; So, R Y; Blinov, V E; Buzykaev, A R; Druzhinin, V P; Golubev, V B; Kozyrev, E A; Kravchenko, E A; Onuchin, A P; Serednyakov, S I; Skovpen, Yu I; Solodov, E P; Todyshev, K Yu; Lankford, A J; Dey, B; Gary, J W; Long, O; Eisner, A M; Lockman, W S; Panduro Vazquez, W; Chao, D S; Cheng, C H; Echenard, B; Flood, K T; Hitlin, D G; Kim, J; Li, Y; Miyashita, T S; Ongmongkolkul, P; Porter, F C; Röhrken, M; Huard, Z; Meadows, B T; Pushpawela, B G; Sokoloff, M D; Sun, L; Smith, J G.
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; Universitat de Barcelona, Facultat de Fisica, Departament ECM, E-08028 Barcelona, Spain.
  • Palano A; INFN Sezione di Bari and Dipartimento di Fisica, Università di Bari, I-70126 Bari, Italy.
  • Eigen G; University of Bergen, Institute of Physics, N-5007 Bergen, Norway.
  • Brown DN; 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.
  • Fritsch M; Ruhr Universität Bochum, Institut für Experimentalphysik 1, D-44780 Bochum, Germany.
  • Koch H; Ruhr Universität Bochum, Institut für Experimentalphysik 1, D-44780 Bochum, Germany.
  • Schroeder T; Ruhr Universität Bochum, Institut für Experimentalphysik 1, D-44780 Bochum, Germany.
  • Hearty C; Institute of Particle Physics, Vancouver, British Columbia, Canada V6T 1Z1.
  • Mattison TS; University of British Columbia, Vancouver, British Columbia, Canada V6T 1Z1.
  • McKenna JA; University of British Columbia, Vancouver, British Columbia, Canada V6T 1Z1.
  • So RY; University of British Columbia, Vancouver, British Columbia, Canada V6T 1Z1.
  • Blinov VE; University of British Columbia, Vancouver, British Columbia, Canada V6T 1Z1.
  • 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.
  • Kozyrev EA; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Kravchenko EA; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Onuchin AP; Novosibirsk State University, Novosibirsk 630090, Russia.
  • Serednyakov SI; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Skovpen YI; Novosibirsk State University, Novosibirsk 630090, Russia.
  • Solodov EP; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Todyshev KY; Novosibirsk State University, Novosibirsk 630090, Russia.
  • Lankford AJ; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Dey B; 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.
  • Eisner AM; Novosibirsk State Technical University, Novosibirsk 630092, Russia.
  • Lockman WS; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Panduro Vazquez W; Novosibirsk State University, Novosibirsk 630090, Russia.
  • Chao DS; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Cheng CH; Novosibirsk State University, Novosibirsk 630090, Russia.
  • Echenard B; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Flood KT; Novosibirsk State University, Novosibirsk 630090, Russia.
  • Hitlin DG; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Kim J; Novosibirsk State University, Novosibirsk 630090, Russia.
  • Li Y; University of California at Irvine, Irvine, California 92697, USA.
  • Miyashita TS; University of California at Riverside, Riverside, California 92521, USA.
  • Ongmongkolkul P; University of California at Riverside, Riverside, California 92521, USA.
  • Porter FC; University of California at Riverside, Riverside, California 92521, USA.
  • Röhrken M; University of California at Santa Cruz, Institute for Particle Physics, Santa Cruz, California 95064, USA.
  • Huard Z; University of California at Santa Cruz, Institute for Particle Physics, Santa Cruz, California 95064, USA.
  • Meadows BT; University of California at Santa Cruz, Institute for Particle Physics, Santa Cruz, California 95064, USA.
  • Pushpawela BG; California Institute of Technology, Pasadena, California 91125, USA.
  • Sokoloff MD; California Institute of Technology, Pasadena, California 91125, USA.
  • Sun L; California Institute of Technology, Pasadena, California 91125, USA.
  • Smith JG; California Institute of Technology, Pasadena, California 91125, USA.
Phys Rev Lett ; 123(9): 091801, 2019 Aug 30.
Article in En | MEDLINE | ID: mdl-31524470
ABSTRACT
An angular analysis of the decay B[over ¯]→D^{*}ℓ^{-}ν[over ¯]_{ℓ}, ℓ∈{e,µ}, is reported using the full e^{+}e^{-} collision data set collected by the BABAR experiment at the ϒ(4S) resonance. One B meson from the ϒ(4S)→BB[over ¯] decay is fully reconstructed in a hadronic decay mode, which constrains the kinematics and provides a determination of the neutrino momentum vector. The kinematics of the semileptonic decay is described by the dilepton mass squared, q^{2}, and three angles. The first unbinned fit to the full four-dimensional decay rate in the standard model is performed in the so-called Boyd-Grinstein-Lebed approach, which employs a generic q^{2} parametrization of the underlying form factors based on crossing symmetry, analyticity, and QCD dispersion relations for the amplitudes. A fit using the more model-dependent Caprini-Lellouch-Neubert (CLN) approach is performed as well. Our form factor shapes show deviations from previous fits based on the CLN parametrization. The latest form factors also provide an updated prediction for the branching fraction ratio R(D^{*})≡B(B[over ¯]→D^{*}τ^{-}ν[over ¯]_{τ})/B(B[over ¯]→D^{*}ℓ^{-}ν[over ¯]_{ℓ})=0.253±0.005. Finally, using the well-measured branching fraction for the B[over ¯]→D^{*}ℓ^{-}ν[over ¯]_{ℓ} decay, a value of |V_{cb}|=(38.36±0.90)×10^{-3} is obtained that is consistent with the current world average for exclusive B[over ¯]→D^{(*)}ℓ^{-}ν[over ¯]_{ℓ} decays and remains in tension with the determination from inclusive semileptonic B decays to final states with charm.

Full text: 1 Collection: 01-internacional Database: MEDLINE Type of study: Prognostic_studies Language: En Journal: Phys Rev Lett Year: 2019 Document type: Article Affiliation country:

Full text: 1 Collection: 01-internacional Database: MEDLINE Type of study: Prognostic_studies Language: En Journal: Phys Rev Lett Year: 2019 Document type: Article Affiliation country: