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First Evidence for cos2ß>0 and Resolution of the Cabibbo-Kobayashi-Maskawa Quark-Mixing Unitarity Triangle Ambiguity.
Adachi, I; Adye, T; Ahmed, H; Ahn, J K; Aihara, H; Akar, S; Alam, M S; Albert, J; Anulli, F; Arnaud, N; Asner, D M; Aston, D; Atmacan, H; Aushev, T; Ayad, R; Babu, V; Badhrees, I; Bakich, A M; Banerjee, Sw; Bansal, V; Barlow, R J; Batignani, G; Beaulieu, A; Behera, P; Bellis, M; Ben-Haim, E; Bernard, D; Bernlochner, F U; Bettarini, S; Bettoni, D; Bevan, A J; Bhardwaj, V; Bhuyan, B; Bianchi, F; Biasini, M; Biswal, J; Blinov, V E; Bomben, M; Bondar, A; Bonneaud, G R; Bozek, A; Bozzi, C; Bracko, M; Browder, T E; Brown, D N; Brown, D N; Bünger, C; Burchat, P R; Buzykaev, A R; Calabrese, R.
Afiliação
  • Adachi I; SOKENDAI (The Graduate University for Advanced Studies), Hayama 240-0193, Japan.
  • Adye T; High Energy Accelerator Research Organization (KEK), Tsukuba 305-0801, Japan.
  • Ahmed H; Rutherford Appleton Laboratory, Chilton, Didcot, Oxon, OX11 0QX, United Kingdom.
  • Ahn JK; St. Francis Xavier University, Antigonish, Nova Scotia, Canada B2G 2W5.
  • Aihara H; Korea University, Seoul 136-713, South Korea.
  • Akar S; Department of Physics, University of Tokyo, Tokyo 113-0033, Japan.
  • Alam MS; Laboratoire de Physique Nucléaire et de Hautes Energies, IN2P3/CNRS, Université Pierre et Marie Curie-Paris6, Université Denis Diderot-Paris7, F-75252 Paris, France.
  • Albert J; State University of New York, Albany, New York 12222, USA.
  • Anulli F; University of Victoria, Victoria, British Columbia, Canada V8W 3P6.
  • Arnaud N; INFN Sezione di Roma, I-00185 Roma, Italy.
  • Asner DM; Laboratoire de l'Accélérateur Linéaire, IN2P3/CNRS et Université Paris-Sud 11, Centre Scientifique d'Orsay, F-91898 Orsay Cedex, France.
  • Aston D; Brookhaven National Laboratory, Upton, New York 11973, USA.
  • Atmacan H; SLAC National Accelerator Laboratory, Stanford, California 94309 USA.
  • Aushev T; University of South Carolina, Columbia, South Carolina 29208, USA.
  • Ayad R; Moscow Institute of Physics and Technology, Moscow Region 141700, Russian Federation.
  • Babu V; Department of Physics, Faculty of Science, University of Tabuk, Tabuk 71451, Kingdom of Saudi Arabia.
  • Badhrees I; Tata Institute of Fundamental Research, Mumbai 400005, India.
  • Bakich AM; King Abdulaziz City for Science and Technology, Riyadh 11442, Kingdom of Saudi Arabia.
  • Banerjee S; Department of Physics, Faculty of Science, University of Tabuk, Tabuk 71451, Kingdom of Saudi Arabia.
  • Bansal V; School of Physics, University of Sydney, New South Wales 2006, Australia.
  • Barlow RJ; University of Louisville, Louisville, Kentucky 40292, USA.
  • Batignani G; Pacific Northwest National Laboratory, Richland, Washington 99352, USA.
  • Beaulieu A; University of Manchester, Manchester M13 9PL, United Kingdom.
  • Behera P; INFN Sezione di Pisa, I-56127 Pisa, Italy.
  • Bellis M; Dipartimento di Fisica, Università di Pisa, I-56127 Pisa, Italy.
  • Ben-Haim E; University of Victoria, Victoria, British Columbia, Canada V8W 3P6.
  • Bernard D; Indian Institute of Technology Madras, Chennai 600036, India.
  • Bernlochner FU; Stanford University, Stanford, California 94305, USA.
  • Bettarini S; Laboratoire de Physique Nucléaire et de Hautes Energies, IN2P3/CNRS, Université Pierre et Marie Curie-Paris6, Université Denis Diderot-Paris7, F-75252 Paris, France.
  • Bettoni D; Laboratoire Leprince-Ringuet, Ecole Polytechnique, CNRS/IN2P3, F-91128 Palaiseau, France.
  • Bevan AJ; University of Victoria, Victoria, British Columbia, Canada V8W 3P6.
  • Bhardwaj V; INFN Sezione di Pisa, I-56127 Pisa, Italy.
  • Bhuyan B; Dipartimento di Fisica, Università di Pisa, I-56127 Pisa, Italy.
  • Bianchi F; INFN Sezione di Ferrara, I-44122 Ferrara, Italy.
  • Biasini M; Queen Mary, University of London, London, E1 4NS, United Kingdom.
  • Biswal J; Indian Institute of Science Education and Research Mohali, SAS Nagar, 140306, India.
  • Blinov VE; Indian Institute of Technology Guwahati, Assam 781039, India.
  • Bomben M; INFN Sezione di Torino, I-10125 Torino, Italy.
  • Bondar A; Dipartimento di Fisica, Università di Torino, I-10125 Torino, Italy.
  • Bonneaud GR; INFN Sezione di Perugia, I-06123 Perugia, Italy.
  • Bozek A; Dipartimento di Fisica, Università di Perugia, I-06123 Perugia, Italy.
  • Bozzi C; J. Stefan Institute, 1000 Ljubljana, Slovenia.
  • Bracko M; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russian Federation.
  • Browder TE; Novosibirsk State University, Novosibirsk 630090, Russian Federation.
  • Brown DN; Novosibirsk State Technical University, Novosibirsk 630092, Russian Federation.
  • Brown DN; Laboratoire de Physique Nucléaire et de Hautes Energies, IN2P3/CNRS, Université Pierre et Marie Curie-Paris6, Université Denis Diderot-Paris7, F-75252 Paris, France.
  • Bünger C; Budker Institute of Nuclear Physics SB RAS, Novosibirsk 630090, Russian Federation.
  • Burchat PR; Novosibirsk State University, Novosibirsk 630090, Russian Federation.
  • Buzykaev AR; Laboratoire de Physique Nucléaire et de Hautes Energies, IN2P3/CNRS, Université Pierre et Marie Curie-Paris6, Université Denis Diderot-Paris7, F-75252 Paris, France.
  • Calabrese R; H. Niewodniczanski Institute of Nuclear Physics, Krakow 31-342, Poland.
Phys Rev Lett ; 121(26): 261801, 2018 Dec 28.
Article em En | MEDLINE | ID: mdl-30636113
ABSTRACT
We present first evidence that the cosine of the CP-violating weak phase 2ß is positive, and hence exclude trigonometric multifold solutions of the Cabibbo-Kobayashi-Maskawa (CKM) Unitarity Triangle using a time-dependent Dalitz plot analysis of B^{0}→D^{(*)}h^{0} with D→K_{S}^{0}π^{+}π^{-} decays, where h^{0}∈{π^{0},η,ω} denotes a light unflavored and neutral hadron. The measurement is performed combining the final data sets of the BABAR and Belle experiments collected at the ϒ(4S) resonance at the asymmetric-energy B factories PEP-II at SLAC and KEKB at KEK, respectively. The data samples contain (471±3)×10^{6}BB[over ¯] pairs recorded by the BABAR detector and (772±11)×10^{6}BB[over ¯] pairs recorded by the Belle detector. The results of the measurement are sin2ß=0.80±0.14(stat)±0.06(syst)±0.03(model) and cos2ß=0.91±0.22(stat)±0.09(syst)±0.07(model). The result for the direct measurement of the angle ß of the CKM Unitarity Triangle is ß=[22.5±4.4(stat)±1.2(syst)±0.6(model)]°. The measurement assumes no direct CP violation in B^{0}→D^{(*)}h^{0} decays. The quoted model uncertainties are due to the composition of the D^{0}→K_{S}^{0}π^{+}π^{-} decay amplitude model, which is newly established by performing a Dalitz plot amplitude analysis using a high-statistics e^{+}e^{-}→cc[over ¯] data sample. CP violation is observed in B^{0}→D^{(*)}h^{0} decays at the level of 5.1 standard deviations. The significance for cos2ß>0 is 3.7 standard deviations. The trigonometric multifold solution π/2-ß=(68.1±0.7)° is excluded at the level of 7.3 standard deviations. The measurement resolves an ambiguity in the determination of the apex of the CKM Unitarity Triangle.

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2018 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2018 Tipo de documento: Article