Measurements of the S-wave fraction in B0 → K+π−μ+μ− decays and the B0 → K∗(892)0μ+μ− differential branching fraction View Full Text


Ontology type: schema:ScholarlyArticle      Open Access: True


Article Info

DATE

2016-11-08

AUTHORS

The LHCb collaboration, R. Aaij, B. Adeva, M. Adinolfi, Z. Ajaltouni, S. Akar, J. Albrecht, F. Alessio, M. Alexander, S. Ali, G. Alkhazov, P. Alvarez Cartelle, A. A. Alves, S. Amato, S. Amerio, Y. Amhis, L. An, L. Anderlini, G. Andreassi, M. Andreotti, J. E. Andrews, R. B. Appleby, O. Aquines Gutierrez, F. Archilli, P. d’Argent, A. Artamonov, M. Artuso, E. Aslanides, G. Auriemma, M. Baalouch, S. Bachmann, J. J. Back, A. Badalov, C. Baesso, W. Baldini, R. J. Barlow, C. Barschel, S. Barsuk, W. Barter, V. Batozskaya, V. Battista, A. Bay, L. Beaucourt, J. Beddow, F. Bedeschi, I. Bediaga, L. J. Bel, V. Bellee, N. Belloli, K. Belous, I. Belyaev, E. Ben-Haim, G. Bencivenni, S. Benson, J. Benton, A. Berezhnoy, R. Bernet, A. Bertolin, M.-O. Bettler, M. van Beuzekom, S. Bifani, P. Billoir, T. Bird, A. Birnkraut, A. Bitadze, A. Bizzeti, T. Blake, F. Blanc, J. Blouw, S. Blusk, V. Bocci, T. Boettcher, A. Bondar, N. Bondar, W. Bonivento, S. Borghi, M. Borisyak, M. Borsato, F. Bossu, M. Boubdir, T. J. V. Bowcock, E. Bowen, C. Bozzi, S. Braun, M. Britsch, T. Britton, J. Brodzicka, E. Buchanan, C. Burr, A. Bursche, J. Buytaert, S. Cadeddu, R. Calabrese, M. Calvi, M. Calvo Gomez, P. Campana, D. Campora Perez, L. Capriotti, A. Carbone, G. Carboni, R. Cardinale, A. Cardini, P. Carniti, L. Carson, K. Carvalho Akiba, G. Casse, L. Cassina, L. Castillo Garcia, M. Cattaneo, Ch. Cauet, G. Cavallero, R. Cenci, M. Charles, Ph. Charpentier, G. Chatzikonstantinidis, M. Chefdeville, S. Chen, S.-F. Cheung, V. Chobanova, M. Chrzaszcz, X. Cid Vidal, G. Ciezarek, P. E. L. Clarke, M. Clemencic, H. V. Cliff, J. Closier, V. Coco, J. Cogan, E. Cogneras, V. Cogoni, L. Cojocariu, G. Collazuol, P. Collins, A. Comerma-Montells, A. Contu, A. Cook, S. Coquereau, G. Corti, M. Corvo, B. Couturier, G. A. Cowan, D. C. Craik, A. Crocombe, M. Cruz Torres, S. Cunliffe, R. Currie, C. D’Ambrosio, E. Dall’Occo, J. Dalseno, P. N. Y. David, A. Davis, O. De Aguiar Francisco, K. De Bruyn, S. De Capua, M. De Cian, J. M. De Miranda, L. De Paula, P. De Simone, C.-T. Dean, D. Decamp, M. Deckenhoff, L. Del Buono, M. Demmer, D. Derkach, O. Deschamps, F. Dettori, B. Dey, A. Di Canto, H. Dijkstra, F. Dordei, M. Dorigo, A. Dosil Suárez, A. Dovbnya, K. Dreimanis, L. Dufour, G. Dujany, K. Dungs, P. Durante, R. Dzhelyadin, A. Dziurda, A. Dzyuba, N. Déléage, S. Easo, U. Egede, V. Egorychev, S. Eidelman, S. Eisenhardt, U. Eitschberger, R. Ekelhof, L. Eklund, Ch. Elsasser, S. Ely, S. Esen, H. M. Evans, T. Evans, A. Falabella, N. Farley, S. Farry, R. Fay, D. Ferguson, V. Fernandez Albor, F. Ferrari, F. Ferreira Rodrigues, M. Ferro-Luzzi, S. Filippov, M. Fiore, M. Fiorini, M. Firlej, C. Fitzpatrick, T. Fiutowski, F. Fleuret, K. Fohl, M. Fontana, F. Fontanelli, D. C. Forshaw, R. Forty, M. Frank, C. Frei, M. Frosini, J. Fu, E. Furfaro, C. Färber, A. Gallas Torreira, D. Galli, S. Gallorini, S. Gambetta, M. Gandelman, P. Gandini, Y. Gao, J. García Pardiñas, J. Garra Tico, L. Garrido, P. J. Garsed, D. Gascon, C. Gaspar, L. Gavardi, G. Gazzoni, D. Gerick, E. Gersabeck, M. Gersabeck, T. Gershon, Ph. Ghez, S. Gianì, V. Gibson, O. G. Girard, L. Giubega, K. Gizdov, V. V. Gligorov, D. Golubkov, A. Golutvin, A. Gomes, I. V. Gorelov, C. Gotti, M. Grabalosa Gándara, R. Graciani Diaz, L. A. Granado Cardoso, E. Graugés, E. Graverini, G. Graziani, A. Grecu, P. Griffith, L. Grillo, O. Grünberg, E. Gushchin, Yu. Guz, T. Gys, C. Göbel, T. Hadavizadeh, C. Hadjivasiliou, G. Haefeli, C. Haen, S. C. Haines, S. Hall, B. Hamilton, X. Han, S. Hansmann-Menzemer, N. Harnew, S. T. Harnew, J. Harrison, J. He, T. Head, A. Heister, K. Hennessy, P. Henrard, L. Henry, J. A. Hernando Morata, E. van Herwijnen, M. Heß, A. Hicheur, D. Hill, C. Hombach, W. Hulsbergen, T. Humair, M. Hushchyn, N. Hussain, D. Hutchcroft, M. Idzik, P. Ilten, R. Jacobsson, A. Jaeger, J. Jalocha, E. Jans, A. Jawahery, M. John, D. Johnson, C. R. Jones, C. Joram, B. Jost, N. Jurik, S. Kandybei, W. Kanso, M. Karacson, T. M. Karbach, S. Karodia, M. Kecke, M. Kelsey, I. R. Kenyon, M. Kenzie, T. Ketel, E. Khairullin, B. Khanji, C. Khurewathanakul, T. Kirn, S. Klaver, K. Klimaszewski, M. Kolpin, I. Komarov, R. F. Koopman, P. Koppenburg, A. Kozachuk, M. Kozeiha, L. Kravchuk, K. Kreplin, M. Kreps, P. Krokovny, F. Kruse, W. Krzemien, W. Kucewicz, M. Kucharczyk, V. Kudryavtsev, A. K. Kuonen, K. Kurek, T. Kvaratskheliya, D. Lacarrere, G. Lafferty, A. Lai, D. Lambert, G. Lanfranchi, C. Langenbruch, B. Langhans, T. Latham, C. Lazzeroni, R. Le Gac, J. van Leerdam, J.-P. Lees, A. Leflat, J. Lefrançois, R. Lefèvre, F. Lemaitre, E. Lemos Cid, O. Leroy, T. Lesiak, B. Leverington, Y. Li, T. Likhomanenko, R. Lindner, C. Linn, F. Lionetto, B. Liu, X. Liu, D. Loh, I. Longstaff, J. H. Lopes, D. Lucchesi, M. Lucio Martinez, H. Luo, A. Lupato, E. Luppi, O. Lupton, A. Lusiani, X. Lyu, F. Machefert, F. Maciuc, O. Maev, K. Maguire, S. Malde, A. Malinin, T. Maltsev, G. Manca, G. Mancinelli, P. Manning, J. Maratas, J. F. Marchand, U. Marconi, C. Marin Benito, P. Marino, J. Marks, G. Martellotti, M. Martin, M. Martinelli, D. Martinez Santos, F. Martinez Vidal, D. Martins Tostes, L. M. Massacrier, A. Massafferri, R. Matev, A. Mathad, Z. Mathe, C. Matteuzzi, A. Mauri, B. Maurin, A. Mazurov, M. McCann, J. McCarthy, A. McNab, R. McNulty, B. Meadows, F. Meier, M. Meissner, D. Melnychuk, M. Merk, E Michielin, D. A. Milanes, M.-N. Minard, D. S. Mitzel, J. Molina Rodriguez, I. A. Monroy, S. Monteil, M. Morandin, P. Morawski, A. Mordà, M. J. Morello, J. Moron, A. B. Morris, R. Mountain, F. Muheim, M. Mulder, M. Mussini, D. Müller, J. Müller, K. Müller, V. Müller, P. Naik, T. Nakada, R. Nandakumar, A. Nandi, I. Nasteva, M. Needham, N. Neri, S. Neubert, N. Neufeld, M. Neuner, A. D. Nguyen, C. Nguyen-Mau, V. Niess, S. Nieswand, R. Niet, N. Nikitin, T. Nikodem, A. Novoselov, D. P. O’Hanlon, A. Oblakowska-Mucha, V. Obraztsov, S. Ogilvy, R. Oldeman, C. J. G. Onderwater, J. M. Otalora Goicochea, A. Otto, P. Owen, A. Oyanguren, A. Palano, F. Palombo, M. Palutan, J. Panman, A. Papanestis, M. Pappagallo, L. L. Pappalardo, C. Pappenheimer, W. Parker, C. Parkes, G. Passaleva, G. D. Patel, M. Patel, C. Patrignani, A. Pearce, A. Pellegrino, G. Penso, M. Pepe Altarelli, S. Perazzini, P. Perret, L. Pescatore, K. Petridis, A. Petrolini, A. Petrov, M. Petruzzo, E. Picatoste Olloqui, B. Pietrzyk, M. Pikies, D. Pinci, A. Pistone, A. Piucci, S. Playfer, M. Plo Casasus, T. Poikela, F. Polci, A. Poluektov, I. Polyakov, E. Polycarpo, G. J. Pomery, A. Popov, D. Popov, B. Popovici, C. Potterat, E. Price, J. D. Price, J. Prisciandaro, A. Pritchard, C. Prouve, V. Pugatch, A. Puig Navarro, G. Punzi, W. Qian, R. Quagliani, B. Rachwal, J. H. Rademacker, M. Rama, M. Ramos Pernas, M. S. Rangel, I. Raniuk, G. Raven, F. Redi, S. Reichert, A. C. dos Reis, C. Remon Alepuz, V. Renaudin, S. Ricciardi, S. Richards, M. Rihl, K. Rinnert, V. Rives Molina, P. Robbe, A. B. Rodrigues, E. Rodrigues, J. A. Rodriguez Lopez, P. Rodriguez Perez, A. Rogozhnikov, S. 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Ward, N. K. Watson, D. Websdale, A. Weiden, M. Whitehead, J. Wicht, G. Wilkinson, M. Wilkinson, M. Williams, M. P. Williams, M. Williams, T. Williams, F. F. Wilson, J. Wimberley, J. Wishahi, W. Wislicki, M. Witek, G. Wormser, S. A. Wotton, K. Wraight, S. Wright, K. Wyllie, Y. Xie, Z. Xing, Z. Xu, Z. Yang, H. Yin, J. Yu, X. Yuan, O. Yushchenko, M. Zangoli, K. A. Zarebski, M. Zavertyaev, L. Zhang, Y. Zhang, Y. Zhang, A. Zhelezov, Y. Zheng, A. Zhokhov, V. Zhukov, S. Zucchelli

ABSTRACT

A measurement of the differential branching fraction of the decay B0 → K∗(892)0μ+μ− is presented together with a determination of the S-wave fraction of the K+π− system in the decay B0 → K+π−μ+μ−. The analysis is based on pp-collision data corresponding to an integrated luminosity of 3 fb−1 collected with the LHCb experiment. The measurements are made in bins of the invariant mass squared of the dimuon system, q2. Precise theoretical predictions for the differential branching fraction of B0 → K∗(892)0μ+μ− decays are available for the q2 region 1.1 < q2< 6.0 GeV2/c4. In this q2 region, for the K+π− invariant mass range 796 < mKπ< 996 MeV/c2, the S-wave fraction of the K+π− system in B0 → K+π−μ+μ− decays is found to be FS=0.101±0.017stat±0.009syst,\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {F}_{\mathrm{S}}=0.101\pm 0.017\left(\mathrm{stat}\right)\pm 0.009\left(\mathrm{syst}\right), $$\end{document} and the differential branching fraction of B0 → K∗(892)0μ+μ− decays is determined to be dℬ/dq2=0.392−0.019+0.020stat±0.010syst±0.027norm×10−7c4/GeV2.\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \mathrm{d}\mathrm{\mathcal{B}}/\mathrm{d}{q}^2=\left(0.{392}_{-0.019}^{+0.020}\left(\mathrm{stat}\right)\pm 0.010\left(\mathrm{syst}\right)\pm 0.027\left(\mathrm{norm}\right)\right)\times 1{0}^{-7}{c}^4/{\mathrm{GeV}}^2. $$\end{document}The differential branching fraction measurements presented are the most precise to date and are found to be in agreement with Standard Model predictions. More... »

PAGES

47

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  • Journal

    TITLE

    Journal of High Energy Physics

    ISSUE

    11

    VOLUME

    2016

    Author Affiliations

  • European Organization for Nuclear Research (CERN), Geneva, Switzerland
  • Universidad de Santiago de Compostela, Santiago de Compostela, Spain
  • H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
  • Clermont Université, Université Blaise Pascal, CNRS/IN2P3, LPC, Clermont-Ferrand, France
  • CPPM, Aix-Marseille Université, CNRS/IN2P3, Marseille, France
  • Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
  • School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
  • Nikhef National Institute for Subatomic Physics, Amsterdam, The Netherlands
  • Petersburg Nuclear Physics Institute (PNPI), Gatchina, Russia
  • Imperial College London, London, United Kingdom
  • University of Cincinnati, Cincinnati, OH, United States
  • Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
  • Sezione INFN di Padova, Padova, Italy
  • LAL, Université Paris-Sud, CNRS/IN2P3, Orsay, France
  • Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
  • Sezione INFN di Firenze, Firenze, Italy
  • Università di Ferrara, Ferrara, Italy
  • University of Maryland, College Park, MD, United States
  • School of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
  • Max-Planck-Institut für Kernphysik (MPIK), Heidelberg, Germany
  • Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
  • Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
  • Institute for High Energy Physics (IHEP), Protvino, Russia
  • Syracuse University, Syracuse, NY, United States
  • Università della Basilicata, Potenza, Italy
  • Department of Physics, University of Warwick, Coventry, United Kingdom
  • Universitat de Barcelona, Barcelona, Spain
  • Pontifícia Universidade Católica do Rio de Janeiro (PUC-Rio), Rio de Janeiro, Brazil
  • Sezione INFN di Ferrara, Ferrara, Italy
  • National Center for Nuclear Research (NCBJ), Warsaw, Poland
  • LAPP, Université Savoie Mont-Blanc, CNRS/IN2P3, Annecy-Le-Vieux, France
  • Sezione INFN di Pisa, Pisa, Italy
  • Università di Milano Bicocca, Milano, Italy
  • Institute of Theoretical and Experimental Physics (ITEP), Moscow, Russia
  • LPNHE, Université Pierre et Marie Curie, Université Paris Diderot, CNRS/IN2P3, Paris, France
  • Laboratori Nazionali dell’INFN di Frascati, Frascati, Italy
  • Institute of Nuclear Physics, Moscow State University (SINP MSU), Moscow, Russia
  • Physik-Institut, Universität Zürich, Zürich, Switzerland
  • University of Birmingham, Birmingham, United Kingdom
  • Università di Modena e Reggio Emilia, Modena, Italy
  • Sezione INFN di Roma La Sapienza, Roma, Italy
  • Massachusetts Institute of Technology, Cambridge, MA, United States
  • Budker Institute of Nuclear Physics (SB RAS) and Novosibirsk State University, Novosibirsk, Russia
  • Sezione INFN di Cagliari, Cagliari, Italy
  • Yandex School of Data Analysis, Moscow, Russia
  • I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
  • Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
  • LIFAELS, La Salle, Universitat Ramon Llull, Barcelona, Spain
  • Università di Bologna, Bologna, Italy
  • Università di Roma Tor Vergata, Roma, Italy
  • Università di Genova, Genova, Italy
  • School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
  • Sezione INFN di Genova, Genova, Italy
  • Scuola Normale Superiore, Pisa, Italy
  • Department of Physics, University of Oxford, Oxford, United Kingdom
  • Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
  • Università di Cagliari, Cagliari, Italy
  • Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest-Magurele, Romania
  • Università di Padova, Padova, Italy
  • Sezione INFN di Milano, Milano, Italy
  • NSC Kharkiv Institute of Physics and Technology (NSC KIPT), Kharkiv, Ukraine
  • STFC Rutherford Appleton Laboratory, Didcot, United Kingdom
  • Sezione INFN di Bologna, Bologna, Italy
  • Institute for Nuclear Research of the Russian Academy of Sciences (INR RAN), Moscow, Russia
  • AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
  • Laboratoire Leprince-Ringuet, Palaiseau, France
  • Università degli Studi di Milano, Milano, Italy
  • Center for High Energy Physics, Tsinghua University, Beijing, China
  • Universidade Federal do Triângulo Mineiro (UFTM), Uberaba, MG, Brazil
  • Sezione INFN di Milano Bicocca, Milano, Italy
  • Institut für Physik, Universität Rostock, Rostock, Germany
  • University of Chinese Academy of Sciences, Beijing, China
  • Nikhef National Institute for Subatomic Physics and VU University Amsterdam, Amsterdam, The Netherlands
  • AGH - University of Science and Technology, Faculty of Computer Science, Electronics and Telecommunications, Kraków, Poland
  • Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
  • National Research Centre Kurchatov Institute, Moscow, Russia
  • Iligan Institute of Technology (IIT), Iligan, Philippines
  • Instituto de Fisica Corpuscular (IFIC), Universitat de Valencia-CSIC, Valencia, Spain
  • School of Physics, University College Dublin, Dublin, Ireland
  • Departamento de Fisica, Universidad Nacional de Colombia, Bogota, Colombia
  • Hanoi University of Science, Hanoi, Viet Nam
  • Van Swinderen Institute, University of Groningen, Groningen, The Netherlands
  • Università di Bari, Bari, Italy
  • Università di Roma La Sapienza, Roma, Italy
  • Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine
  • Università di Pisa, Pisa, Italy
  • Sezione INFN di Roma Tor Vergata, Roma, Italy
  • Università di Urbino, Urbino, Italy
  • Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
  • P.N. Lebedev Physical Institute, Russian Academy of Science (LPI RAS), Moscow, Russia
  • Identifiers

    URI

    http://scigraph.springernature.com/pub.10.1007/jhep11(2016)047

    DOI

    http://dx.doi.org/10.1007/jhep11(2016)047

    DIMENSIONS

    https://app.dimensions.ai/details/publication/pub.1003744131


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    25 schema:description A measurement of the differential branching fraction of the decay B0 → K∗(892)0μ+μ− is presented together with a determination of the S-wave fraction of the K+π− system in the decay B0 → K+π−μ+μ−. The analysis is based on pp-collision data corresponding to an integrated luminosity of 3 fb−1 collected with the LHCb experiment. The measurements are made in bins of the invariant mass squared of the dimuon system, q2. Precise theoretical predictions for the differential branching fraction of B0 → K∗(892)0μ+μ− decays are available for the q2 region 1.1 < q2< 6.0 GeV2/c4. In this q2 region, for the K+π− invariant mass range 796 < mKπ< 996 MeV/c2, the S-wave fraction of the K+π− system in B0 → K+π−μ+μ− decays is found to be FS=0.101±0.017stat±0.009syst,\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {F}_{\mathrm{S}}=0.101\pm 0.017\left(\mathrm{stat}\right)\pm 0.009\left(\mathrm{syst}\right), $$\end{document} and the differential branching fraction of B0 → K∗(892)0μ+μ− decays is determined to be dℬ/dq2=0.392−0.019+0.020stat±0.010syst±0.027norm×10−7c4/GeV2.\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \mathrm{d}\mathrm{\mathcal{B}}/\mathrm{d}{q}^2=\left(0.{392}_{-0.019}^{+0.020}\left(\mathrm{stat}\right)\pm 0.010\left(\mathrm{syst}\right)\pm 0.027\left(\mathrm{norm}\right)\right)\times 1{0}^{-7}{c}^4/{\mathrm{GeV}}^2. $$\end{document}The differential branching fraction measurements presented are the most precise to date and are found to be in agreement with Standard Model predictions.
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