Angular analysis of B0→D∗−Ds∗+ with Ds∗+→Ds+γ decays View Full Text


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DATE

2021-06-29

AUTHORS

R. Aaij, C. Abellán Beteta, T. Ackernley, B. Adeva, M. Adinolfi, H. Afsharnia, C. A. Aidala, S. Aiola, Z. Ajaltouni, S. Akar, J. Albrecht, F. Alessio, M. Alexander, A. Alfonso Albero, Z. Aliouche, G. Alkhazov, P. Alvarez Cartelle, S. Amato, Y. Amhis, L. An, L. Anderlini, A. Andreianov, M. Andreotti, F. Archilli, A. Artamonov, M. Artuso, K. Arzymatov, E. Aslanides, M. Atzeni, B. Audurier, S. Bachmann, M. Bachmayer, J. J. Back, P. Baladron Rodriguez, V. Balagura, W. Baldini, J. Baptista Leite, R. J. Barlow, S. Barsuk, W. Barter, M. Bartolini, F. Baryshnikov, J. M. Basels, G. Bassi, B. Batsukh, A. Battig, A. Bay, M. Becker, F. Bedeschi, I. Bediaga, A. Beiter, V. Belavin, S. Belin, V. Bellee, K. Belous, I. Belov, I. Belyaev, G. Bencivenni, E. Ben-Haim, A. Berezhnoy, R. Bernet, D. Berninghoff, H. C. Bernstein, C. Bertella, A. Bertolin, C. Betancourt, F. Betti, Ia. Bezshyiko, S. Bhasin, J. Bhom, L. Bian, M. S. Bieker, S. Bifani, P. Billoir, M. Birch, F. C. R. Bishop, A. Bitadze, A. Bizzeti, M. Bjørn, M. P. Blago, T. Blake, F. Blanc, S. Blusk, D. Bobulska, J. A. Boelhauve, O. Boente Garcia, T. Boettcher, A. Boldyrev, A. Bondar, N. Bondar, S. Borghi, M. Borisyak, M. Borsato, J. T. Borsuk, S. A. Bouchiba, T. J. V. Bowcock, A. Boyer, C. Bozzi, M. J. Bradley, S. Braun, A. Brea Rodriguez, M. Brodski, J. Brodzicka, A. Brossa Gonzalo, D. Brundu, A. Buonaura, C. Burr, A. Bursche, A. Butkevich, J. S. Butter, J. Buytaert, W. Byczynski, S. Cadeddu, H. Cai, R. Calabrese, L. Calefice, L. Calero Diaz, S. Cali, R. Calladine, M. Calvi, M. Calvo Gomez, P. Camargo Magalhaes, A. Camboni, P. Campana, A. F. Campoverde Quezada, S. Capelli, L. Capriotti, A. Carbone, G. Carboni, R. Cardinale, A. Cardini, I. Carli, P. Carniti, L. Carus, K. Carvalho Akiba, A. Casais Vidal, G. Casse, M. Cattaneo, G. Cavallero, S. Celani, J. Cerasoli, A. J. Chadwick, M. G. Chapman, M. Charles, Ph. Charpentier, G. Chatzikonstantinidis, C. A. Chavez Barajas, M. Chefdeville, C. Chen, S. Chen, A. Chernov, V. Chobanova, S. Cholak, M. Chrzaszcz, A. Chubykin, V. Chulikov, P. Ciambrone, M. F. Cicala, X. Cid Vidal, G. Ciezarek, P. E. L. Clarke, M. Clemencic, H. V. Cliff, J. Closier, J. L. Cobbledick, V. Coco, J. A. B. Coelho, J. Cogan, E. Cogneras, L. Cojocariu, P. Collins, T. Colombo, L. Congedo, A. Contu, N. Cooke, G. Coombs, G. Corti, C. M. Costa Sobral, B. Couturier, D. C. Craik, J. Crkovská, M. Cruz Torres, R. Currie, C. L. Da Silva, E. Dall’Occo, J. Dalseno, C. D’Ambrosio, A. Danilina, P. d’Argent, A. Davis, O. De Aguiar Francisco, K. De Bruyn, S. De Capua, M. De Cian, J. M. De Miranda, L. De Paula, M. De Serio, D. De Simone, P. De Simone, J. A. de Vries, C. T. Dean, D. Decamp, L. Del Buono, B. Delaney, H.-P. Dembinski, A. Dendek, V. Denysenko, D. Derkach, O. Deschamps, F. Desse, F. Dettori, B. Dey, P. Di Nezza, S. Didenko, L. Dieste Maronas, H. Dijkstra, V. Dobishuk, A. M. Donohoe, F. Dordei, A. C. dos Reis, L. Douglas, A. Dovbnya, A. G. Downes, K. Dreimanis, M. W. Dudek, L. Dufour, V. Duk, P. Durante, J. M. Durham, D. Dutta, A. Dziurda, A. Dzyuba, S. Easo, U. Egede, V. Egorychev, S. Eidelman, S. Eisenhardt, S. Ek-In, L. Eklund, S. Ely, A. Ene, E. Epple, S. Escher, J. Eschle, S. Esen, T. Evans, A. Falabella, J. Fan, Y. Fan, B. Fang, S. Farry, D. Fazzini, M. Féo, A. Fernandez Prieto, J. M. Fernandez-tenllado Arribas, A. D. Fernez, F. Ferrari, L. Ferreira Lopes, F. Ferreira Rodrigues, S. Ferreres Sole, M. Ferrillo, M. Ferro-Luzzi, S. Filippov, R. A. Fini, M. Fiorini, M. Firlej, K. M. Fischer, D. S. Fitzgerald, C. Fitzpatrick, T. Fiutowski, F. Fleuret, M. Fontana, F. Fontanelli, R. Forty, V. Franco Lima, M. Franco Sevilla, M. Frank, E. Franzoso, G. Frau, C. Frei, D. A. Friday, J. Fu, Q. Fuehring, W. Funk, E. Gabriel, T. Gaintseva, A. Gallas Torreira, D. Galli, S. Gambetta, Y. Gan, M. Gandelman, P. Gandini, Y. Gao, M. Garau, L. M. Garcia Martin, P. Garcia Moreno, J. García Pardiñas, B. Garcia Plana, F. A. Garcia Rosales, L. Garrido, C. Gaspar, R. E. Geertsema, D. Gerick, L. L. Gerken, E. Gersabeck, M. Gersabeck, T. Gershon, D. Gerstel, Ph. Ghez, V. Gibson, H. K. Giemza, M. Giovannetti, A. Gioventù, P. Gironella Gironell, L. Giubega, C. Giugliano, K. Gizdov, E. L. Gkougkousis, V. V. Gligorov, C. Göbel, E. Golobardes, D. Golubkov, A. Golutvin, A. Gomes, S. Gomez Fernandez, F. Goncalves Abrantes, M. Goncerz, G. Gong, P. Gorbounov, I. V. Gorelov, C. Gotti, E. Govorkova, J. P. Grabowski, T. Grammatico, L. A. Granado Cardoso, E. Graugés, E. Graverini, G. Graziani, A. Grecu, L. M. Greeven, P. Griffith, L. Grillo, S. Gromov, B. R. Gruberg Cazon, C. Gu, M. Guarise, P. A. Günther, E. Gushchin, A. Guth, Y. Guz, T. Gys, T. Hadavizadeh, G. Haefeli, C. Haen, J. Haimberger, T. Halewood-leagas, P. M. Hamilton, J. P. Hammerich, Q. Han, X. Han, T. H. Hancock, S. Hansmann-Menzemer, N. Harnew, T. Harrison, C. Hasse, M. Hatch, J. He, M. Hecker, K. Heijhoff, K. Heinicke, A. M. Hennequin, K. Hennessy, L. Henry, J. Heuel, A. Hicheur, D. Hill, M. Hilton, S. E. Hollitt, J. Hu, J. Hu, W. Hu, W. Huang, X. Huang, W. Hulsbergen, R. J. Hunter, M. Hushchyn, D. Hutchcroft, D. Hynds, P. Ibis, M. Idzik, D. Ilin, P. Ilten, A. Inglessi, A. Ishteev, K. Ivshin, R. Jacobsson, S. Jakobsen, E. Jans, B. K. Jashal, A. Jawahery, V. Jevtic, M. Jezabek, F. Jiang, M. John, D. Johnson, C. R. Jones, T. P. Jones, B. Jost, N. Jurik, S. Kandybei, Y. Kang, M. Karacson, M. Karpov, F. Keizer, M. Kenzie, T. Ketel, B. Khanji, A. Kharisova, S. Kholodenko, T. Kirn, V. S. Kirsebom, O. Kitouni, S. Klaver, K. Klimaszewski, S. Koliiev, A. Kondybayeva, A. Konoplyannikov, P. Kopciewicz, R. Kopecna, P. Koppenburg, M. Korolev, I. Kostiuk, O. Kot, S. Kotriakhova, P. Kravchenko, L. Kravchuk, R. D. Krawczyk, M. Kreps, F. Kress, S. Kretzschmar, P. Krokovny, W. Krupa, W. Krzemien, W. Kucewicz, M. Kucharczyk, V. Kudryavtsev, H. S. Kuindersma, G. J. Kunde, T. Kvaratskheliya, D. Lacarrere, G. Lafferty, A. Lai, A. Lampis, D. Lancierini, J. J. Lane, R. Lane, G. Lanfranchi, C. Langenbruch, J. Langer, O. Lantwin, T. Latham, F. Lazzari, R. Le Gac, S. H. Lee, R. Lefèvre, A. Leflat, S. Legotin, O. Leroy, T. Lesiak, B. Leverington, H. Li, L. Li, P. Li, S. Li, Y. Li, Y. Li, Z. Li, X. Liang, T. Lin, R. Lindner, V. Lisovskyi, R. Litvinov, G. Liu, H. Liu, S. Liu, X. Liu, A. Loi, J. Lomba Castro, I. Longstaff, J. H. Lopes, G. H. Lovell, Y. Lu, D. Lucchesi, S. Luchuk, M. Lucio Martinez, V. Lukashenko, Y. Luo, A. Lupato, E. Luppi, O. Lupton, A. Lusiani, X. Lyu, L. Ma, R. Ma, S. Maccolini, F. Machefert, F. Maciuc, V. Macko, P. Mackowiak, S. Maddrell-Mander, O. Madejczyk, L. R. Madhan Mohan, O. Maev, A. Maevskiy, D. Maisuzenko, M. W. Majewski, J. J. Malczewski, S. Malde, B. Malecki, A. Malinin, T. Maltsev, H. Malygina, G. Manca, G. Mancinelli, D. Manuzzi, D. Marangotto, J. Maratas, J. F. Marchand, U. Marconi, S. Mariani, C. Marin Benito, M. Marinangeli, J. Marks, A. M. Marshall, P. J. Marshall, G. Martellotti, L. Martinazzoli, M. Martinelli, D. Martinez Santos, F. Martinez Vidal, A. 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ABSTRACT

The first full angular analysis of the B0→D∗−Ds∗+\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {B}^0\to {D}^{\ast -}{D}_s^{\ast +} $$\end{document} decay is performed using 6 fb−1 of pp collision data collected with the LHCb experiment at a centre-of-mass energy of 13 TeV. The Ds∗+→Ds+γ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {D}_s^{\ast +}\to {D}_s^{+}\gamma $$\end{document} and D*− → D¯0π−\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {\overline{D}}^0{\pi}^{-} $$\end{document} vector meson decays are used with the subsequent Ds+\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {D}_s^{+} $$\end{document} → K+K−π+ and D¯0\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {\overline{D}}^0 $$\end{document} → K+π− decays. All helicity amplitudes and phases are measured, and the longitudinal polarisation fraction is determined to be fL = 0.578 ± 0.010 ± 0.011 with world-best precision, where the first uncertainty is statistical and the second is systematic. The pattern of helicity amplitude magnitudes is found to align with expectations from quark-helicity conservation in B decays. The ratio of branching fractions [ℬ(B0→D∗−Ds∗+\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {B}^0\to {D}^{\ast -}{D}_s^{\ast +} $$\end{document}) × ℬ(Ds∗+→Ds+γ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {D}_s^{\ast +}\to {D}_s^{+}\gamma $$\end{document})]/ℬ(B0 → D*−Ds+\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {D}_s^{+} $$\end{document}) is measured to be 2.045 ± 0.022 ± 0.071 with world-best precision. In addition, the first observation of the Cabibbo-suppressed Bs → D*−Ds+\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {D}_s^{+} $$\end{document} decay is made with a significance of seven standard deviations. The branching fraction ratio ℬ(Bs → D*−Ds+\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {D}_s^{+} $$\end{document})/ℬ(B0 → D*−Ds+\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {D}_s^{+} $$\end{document}) is measured to be 0.049 ± 0.006 ± 0.003 ± 0.002, where the third uncertainty is due to limited knowledge of the ratio of fragmentation fractions. More... »

PAGES

177

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  • Journal

    TITLE

    Journal of High Energy Physics

    ISSUE

    6

    VOLUME

    2021

    Author Affiliations

  • Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
  • Physik-Institut, Universität Zürich, Zürich, Switzerland
  • Oliver Lodge Laboratory, University of Liverpool, Liverpool, U.K.
  • Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
  • H.H. Wills Physics Laboratory, University of Bristol, Bristol, U.K.
  • Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
  • University of Michigan, Ann Arbor, United States
  • INFN Sezione di Milano, Milano, Italy
  • University of Cincinnati, Cincinnati, OH, United States
  • Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
  • European Organization for Nuclear Research (CERN), Geneva, Switzerland
  • School of Physics and Astronomy, University of Glasgow, Glasgow, U.K.
  • ICCUB, Universitat de Barcelona, Barcelona, Spain
  • Department of Physics and Astronomy, University of Manchester, Manchester, U.K.
  • Petersburg Nuclear Physics Institute NRC Kurchatov Institute (PNPI NRC KI), Gatchina, Russia
  • Cavendish Laboratory, University of Cambridge, Cambridge, U.K.
  • Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
  • Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
  • INFN Sezione di Firenze, Firenze, Italy
  • INFN Sezione di Ferrara, Ferrara, Italy
  • Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
  • Institute for High Energy Physics NRC Kurchatov Institute (IHEP NRC KI), Protvino, Russia
  • Syracuse University, Syracuse, NY, United States
  • Yandex School of Data Analysis, Moscow, Russia
  • Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
  • Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France
  • Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
  • Department of Physics, University of Warwick, Coventry, U.K.
  • Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
  • Imperial College London, London, U.K.
  • INFN Sezione di Genova, Genova, Italy
  • National University of Science and Technology “MISIS”, Moscow, Russia
  • I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
  • INFN Sezione di Pisa, Pisa, Italy
  • INFN Sezione di Cagliari, Monserrato, Italy
  • Institute of Nuclear Physics, Moscow State University (SINP MSU), Moscow, Russia
  • Institute of Theoretical and Experimental Physics NRC Kurchatov Institute (ITEP NRC KI), Moscow, Russia
  • INFN Laboratori Nazionali di Frascati, Frascati, Italy
  • LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
  • Universita degli Studi di Padova, Universita e INFN, Padova, Padova, Italy
  • Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
  • School of Physics and Technology, Wuhan University, Wuhan, China
  • University of Birmingham, Birmingham, U.K.
  • Università di Modena e Reggio Emilia, Modena, Italy
  • Department of Physics, University of Oxford, Oxford, U.K.
  • National Research University Higher School of Economics, Moscow, Russia
  • Budker Institute of Nuclear Physics (SB RAS), Novosibirsk, Russia
  • University of Maryland, College Park, MD, United States
  • Guangdong Provencial Key Laboratory of Nuclear Science, Institute of Quantum Matter, South China Normal University, Guangzhou, China
  • Institute for Nuclear Research of the Russian Academy of Sciences (INR RAS), Moscow, Russia
  • Università di Ferrara, Ferrara, Italy
  • Università di Milano Bicocca, Milano, Italy
  • DS4DS, La Salle, Universitat Ramon Llull, Barcelona, Spain
  • University of Chinese Academy of Sciences, Beijing, China
  • Università di Bologna, Bologna, Italy
  • INFN Sezione di Roma Tor Vergata, Roma, Italy
  • Institute Of High Energy Physics (IHEP), Beijing, China
  • Univ. Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France
  • Center for High Energy Physics, Tsinghua University, Beijing, China
  • School of Physics and Astronomy, University of Edinburgh, Edinburgh, U.K.
  • Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest-Magurele, Romania
  • Università di Bari, Bari, Italy
  • Massachusetts Institute of Technology, Cambridge, MA, United States
  • Los Alamos National Laboratory (LANL), Los Alamos, United States
  • Van Swinderen Institute, University of Groningen, Groningen, Netherlands
  • Universiteit Maastricht, Maastricht, Netherlands
  • AGH — University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
  • Università di Cagliari, Cagliari, Italy
  • Eotvos Lorand University, Budapest, Hungary
  • Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine
  • School of Physics, University College Dublin, Dublin, Ireland
  • NSC Kharkiv Institute of Physics and Technology (NSC KIPT), Kharkiv, Ukraine
  • INFN Sezione di Perugia, Perugia, Italy
  • STFC Rutherford Appleton Laboratory, Didcot, U.K.
  • School of Physics and Astronomy, Monash University, Melbourne, Australia
  • Novosibirsk State University, Novosibirsk, Russia
  • Department of Physics and Astronomy, Uppsala University, Uppsala, Sweden
  • INFN Sezione di Bologna, Bologna, Italy
  • INFN Sezione di Bari, Bari, Italy
  • Università di Genova, Genova, Italy
  • School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
  • National Center for Nuclear Research (NCBJ), Warsaw, Poland
  • Università di Roma Tor Vergata, Roma, Italy
  • Pontifícia Universidade Católica do Rio de Janeiro (PUC-Rio), Rio de Janeiro, Brazil
  • Universidade Federal do Triângulo Mineiro (UFTM), Uberaba, MG, Brazil
  • INFN Sezione di Milano-Bicocca, Milano, Italy
  • Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
  • Hangzhou Institute for Advanced Study, UCAS, Hangzhou, China
  • Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia — CSIC, Valencia, Spain
  • Nikhef National Institute for Subatomic Physics and VU University Amsterdam, Amsterdam, Netherlands
  • National Research Tomsk Polytechnic University, Tomsk, Russia
  • AGH — University of Science and Technology, Faculty of Computer Science, Electronics and Telecommunications, Kraków, Poland
  • Università di Siena, Siena, Italy
  • Università di Padova, Padova, Italy
  • Scuola Normale Superiore, Pisa, Italy
  • National Research Centre Kurchatov Institute, Moscow, Russia
  • Università degli Studi di Milano, Milano, Italy
  • MSU — Iligan Institute of Technology (MSU-IIT), Iligan, Philippines
  • Università di Firenze, Firenze, Italy
  • INFN Sezione di Roma La Sapienza, Roma, Italy
  • Institut für Physik, Universität Rostock, Rostock, Germany
  • Departamento de Fisica, Universidad Nacional de Colombia, Bogota, Colombia
  • Universität Bonn — Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany
  • Hanoi University of Science, Hanoi, Vietnam
  • Università di Pisa, Pisa, Italy
  • P.N. Lebedev Physical Institute, Russian Academy of Science (LPI RAS), Moscow, Russia
  • Università della Basilicata, Potenza, Italy
  • Max-Planck-Institut für Kernphysik (MPIK), Heidelberg, Germany
  • Università di Urbino, Urbino, Italy
  • Physics and Micro Electronic College, Hunan University, Changsha City, China
  • Identifiers

    URI

    http://scigraph.springernature.com/pub.10.1007/jhep06(2021)177

    DOI

    http://dx.doi.org/10.1007/jhep06(2021)177

    DIMENSIONS

    https://app.dimensions.ai/details/publication/pub.1139278529


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The Ds\u2217+\u2192Ds+\u03b3\\documentclass[12pt]{minimal}\n\t\t\t\t\\usepackage{amsmath}\n\t\t\t\t\\usepackage{wasysym}\n\t\t\t\t\\usepackage{amsfonts}\n\t\t\t\t\\usepackage{amssymb}\n\t\t\t\t\\usepackage{amsbsy}\n\t\t\t\t\\usepackage{mathrsfs}\n\t\t\t\t\\usepackage{upgreek}\n\t\t\t\t\\setlength{\\oddsidemargin}{-69pt}\n\t\t\t\t\\begin{document}$$ {D}_s^{\\ast +}\\to {D}_s^{+}\\gamma $$\\end{document} and D*\u2212 \u2192 D\u00af0\u03c0\u2212\\documentclass[12pt]{minimal}\n\t\t\t\t\\usepackage{amsmath}\n\t\t\t\t\\usepackage{wasysym}\n\t\t\t\t\\usepackage{amsfonts}\n\t\t\t\t\\usepackage{amssymb}\n\t\t\t\t\\usepackage{amsbsy}\n\t\t\t\t\\usepackage{mathrsfs}\n\t\t\t\t\\usepackage{upgreek}\n\t\t\t\t\\setlength{\\oddsidemargin}{-69pt}\n\t\t\t\t\\begin{document}$$ {\\overline{D}}^0{\\pi}^{-} $$\\end{document} vector meson decays are used with the subsequent Ds+\\documentclass[12pt]{minimal}\n\t\t\t\t\\usepackage{amsmath}\n\t\t\t\t\\usepackage{wasysym}\n\t\t\t\t\\usepackage{amsfonts}\n\t\t\t\t\\usepackage{amssymb}\n\t\t\t\t\\usepackage{amsbsy}\n\t\t\t\t\\usepackage{mathrsfs}\n\t\t\t\t\\usepackage{upgreek}\n\t\t\t\t\\setlength{\\oddsidemargin}{-69pt}\n\t\t\t\t\\begin{document}$$ {D}_s^{+} $$\\end{document} \u2192 K+K\u2212\u03c0+ and D\u00af0\\documentclass[12pt]{minimal}\n\t\t\t\t\\usepackage{amsmath}\n\t\t\t\t\\usepackage{wasysym}\n\t\t\t\t\\usepackage{amsfonts}\n\t\t\t\t\\usepackage{amssymb}\n\t\t\t\t\\usepackage{amsbsy}\n\t\t\t\t\\usepackage{mathrsfs}\n\t\t\t\t\\usepackage{upgreek}\n\t\t\t\t\\setlength{\\oddsidemargin}{-69pt}\n\t\t\t\t\\begin{document}$$ {\\overline{D}}^0 $$\\end{document} \u2192 K+\u03c0\u2212 decays. All helicity amplitudes and phases are measured, and the longitudinal polarisation fraction is determined to be fL = 0.578 \u00b1 0.010 \u00b1 0.011 with world-best precision, where the first uncertainty is statistical and the second is systematic. The pattern of helicity amplitude magnitudes is found to align with expectations from quark-helicity conservation in B decays. The ratio of branching fractions [\u212c(B0\u2192D\u2217\u2212Ds\u2217+\\documentclass[12pt]{minimal}\n\t\t\t\t\\usepackage{amsmath}\n\t\t\t\t\\usepackage{wasysym}\n\t\t\t\t\\usepackage{amsfonts}\n\t\t\t\t\\usepackage{amssymb}\n\t\t\t\t\\usepackage{amsbsy}\n\t\t\t\t\\usepackage{mathrsfs}\n\t\t\t\t\\usepackage{upgreek}\n\t\t\t\t\\setlength{\\oddsidemargin}{-69pt}\n\t\t\t\t\\begin{document}$$ {B}^0\\to {D}^{\\ast -}{D}_s^{\\ast +} $$\\end{document}) \u00d7 \u212c(Ds\u2217+\u2192Ds+\u03b3\\documentclass[12pt]{minimal}\n\t\t\t\t\\usepackage{amsmath}\n\t\t\t\t\\usepackage{wasysym}\n\t\t\t\t\\usepackage{amsfonts}\n\t\t\t\t\\usepackage{amssymb}\n\t\t\t\t\\usepackage{amsbsy}\n\t\t\t\t\\usepackage{mathrsfs}\n\t\t\t\t\\usepackage{upgreek}\n\t\t\t\t\\setlength{\\oddsidemargin}{-69pt}\n\t\t\t\t\\begin{document}$$ {D}_s^{\\ast +}\\to {D}_s^{+}\\gamma $$\\end{document})]/\u212c(B0 \u2192 D*\u2212Ds+\\documentclass[12pt]{minimal}\n\t\t\t\t\\usepackage{amsmath}\n\t\t\t\t\\usepackage{wasysym}\n\t\t\t\t\\usepackage{amsfonts}\n\t\t\t\t\\usepackage{amssymb}\n\t\t\t\t\\usepackage{amsbsy}\n\t\t\t\t\\usepackage{mathrsfs}\n\t\t\t\t\\usepackage{upgreek}\n\t\t\t\t\\setlength{\\oddsidemargin}{-69pt}\n\t\t\t\t\\begin{document}$$ {D}_s^{+} $$\\end{document}) is measured to be 2.045 \u00b1 0.022 \u00b1 0.071 with world-best precision. In addition, the first observation of the Cabibbo-suppressed Bs \u2192 D*\u2212Ds+\\documentclass[12pt]{minimal}\n\t\t\t\t\\usepackage{amsmath}\n\t\t\t\t\\usepackage{wasysym}\n\t\t\t\t\\usepackage{amsfonts}\n\t\t\t\t\\usepackage{amssymb}\n\t\t\t\t\\usepackage{amsbsy}\n\t\t\t\t\\usepackage{mathrsfs}\n\t\t\t\t\\usepackage{upgreek}\n\t\t\t\t\\setlength{\\oddsidemargin}{-69pt}\n\t\t\t\t\\begin{document}$$ {D}_s^{+} $$\\end{document} decay is made with a significance of seven standard deviations. 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