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Observation of the Decay 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; 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; Wagner, S R.
Afiliação
  • 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.
  • Gary JW; Novosibirsk State University, Novosibirsk 630090, Russia.
  • Long O; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Eisner AM; Novosibirsk State University, Novosibirsk 630090, Russia.
  • Lockman WS; Novosibirsk State Technical University, Novosibirsk 630092, Russia.
  • Panduro Vazquez W; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Chao DS; Novosibirsk State University, Novosibirsk 630090, Russia.
  • Cheng CH; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Echenard B; Novosibirsk State University, Novosibirsk 630090, Russia.
  • Flood KT; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Hitlin DG; Novosibirsk State University, Novosibirsk 630090, Russia.
  • Kim J; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russia.
  • Li Y; Novosibirsk State University, Novosibirsk 630090, Russia.
  • Miyashita TS; University of California at Irvine, Irvine, California 92697, 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.
  • Wagner SR; California Institute of Technology, Pasadena, California 91125, USA.
Phys Rev Lett ; 122(8): 081802, 2019 Mar 01.
Article em En | MEDLINE | ID: mdl-30932586
ABSTRACT
We report the observation of the rare charm decay D^{0}→K^{-}π^{+}e^{+}e^{-}, based on 468 fb^{-1} of e^{+}e^{-} annihilation data collected at or close to the center-of-mass energy of the ϒ(4S) resonance with the BABAR detector at the SLAC National Accelerator Laboratory. We find the branching fraction in the invariant mass range 0.675electron-positron pair to be B(D^{0}→K^{-}π^{+}e^{+}e^{-})=(4.0±0.5±0.2±0.1)×10^{-6}, where the first uncertainty is statistical, the second systematic, and the third due to the uncertainty in the branching fraction of the decay D^{0}→K^{-}π^{+}π^{+}π^{-} used as a normalization mode. The significance of the observation corresponds to 9.7 standard deviations including systematic uncertainties. This result is consistent with the recently reported D^{0}→K^{-}π^{+}µ^{+}µ^{-} branching fraction, measured in the same invariant mass range, and with the value expected in the standard model. In a set of regions of m(e^{+}e^{-}), where long-distance effects are potentially small, we determine a 90% confidence level upper limit on the branching fraction B(D^{0}→K^{-}π^{+}e^{+}e^{-})<3.1×10^{-6}.

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2019 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2019 Tipo de documento: Article