Study of the ψ2(3823) and χc1(3872) states in B+→ (J/ψπ+π−)K+ decays View Full Text


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DATE

2020-08-25

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, A. A. Alves, S. Amato, Y. Amhis, L. An, L. Anderlini, G. Andreassi, 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, S. Baker, 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, V. Batozskaya, B. Batsukh, A. Battig, A. Bay, M. Becker, F. Bedeschi, I. Bediaga, A. Beiter, V. Belavin, S. Belin, V. Bellee, K. Belous, I. Belyaev, G. Bencivenni, E. Ben-Haim, A. Berezhnoy, R. Bernet, D. Berninghoff, H. C. Bernstein, C. Bertella, E. Bertholet, A. Bertolin, C. Betancourt, F. Betti, M. O. Bettler, Ia. Bezshyiko, S. Bhasin, J. Bhom, L. Bian, M. S. Bieker, S. Bifani, P. Billoir, F. C. R. Bishop, A. Bizzeti, M. Bjørn, M. P. Blago, T. Blake, F. Blanc, S. Blusk, D. Bobulska, V. Bocci, 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, E. Buchanan, A. Buonaura, C. Burr, A. Bursche, A. Butkevich, J. S. Butter, J. Buytaert, W. Byczynski, S. Cadeddu, H. Cai, R. Calabrese, L. Calero Diaz, S. Cali, R. Calladine, M. Calvi, M. Calvo Gomez, P. Camargo Magalhaes, A. Camboni, P. Campana, D. H. Campora Perez, A. F. Campoverde Quezada, S. Capelli, L. Capriotti, A. Carbone, G. Carboni, R. Cardinale, A. Cardini, I. Carli, P. Carniti, K. Carvalho Akiba, A. Casais Vidal, G. Casse, M. Cattaneo, G. Cavallero, S. Celani, R. Cenci, J. Cerasoli, A. J. Chadwick, M. G. Chapman, M. Charles, Ph. Charpentier, G. Chatzikonstantinidis, M. Chefdeville, C. Chen, S. Chen, A. Chernov, S.-G. Chitic, V. Chobanova, S. Cholak, M. Chrzaszcz, A. Chubykin, V. Chulikov, P. Ciambrone, M. F. Cicala, X. Cid Vidal, G. Ciezarek, F. Cindolo, 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, A. Contu, N. Cooke, G. Coombs, S. Coquereau, 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, W. 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, A. Di Canto, P. Di Nezza, S. Didenko, H. Dijkstra, V. Dobishuk, A. M. Donohoe, F. Dordei, M. Dorigo, A. C. dos Reis, L. Douglas, A. Dovbnya, A. G. Downes, K. Dreimanis, M. W. Dudek, L. Dufour, P. Durante, J. M. Durham, D. Dutta, M. Dziewiecki, 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, N. Farley, S. Farry, D. Fazzini, P. Fedin, M. Féo, P. Fernandez Declara, A. Fernandez Prieto, 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, 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. Gallorini, 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, D. Gascon, C. Gaspar, R. E. Geertsema, D. Gerick, E. Gersabeck, M. Gersabeck, T. Gershon, D. Gerstel, Ph. Ghez, V. Gibson, A. Gioventù, P. Gironella Gironell, L. Giubega, C. Giugliano, K. Gizdov, V. V. Gligorov, C. Göbel, E. Golobardes, D. Golubkov, A. Golutvin, A. Gomes, M. Goncerz, P. Gorbounov, I. V. Gorelov, C. Gotti, E. Govorkova, J. P. Grabowski, R. Graciani Diaz, T. Grammatico, L. A. Granado Cardoso, E. Graugés, E. Graverini, G. Graziani, A. Grecu, L. M. Greeven, P. Griffith, L. Grillo, L. Gruber, B. R. Gruberg Cazon, C. Gu, M. Guarise, P. A. Günther, E. Gushchin, A. Guth, Yu. Guz, T. Gys, T. Hadavizadeh, G. Haefeli, C. Haen, S. C. Haines, P. M. Hamilton, Q. Han, X. Han, T. H. Hancock, S. Hansmann-Menzemer, N. Harnew, T. Harrison, R. Hart, 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, P. H. Hopchev, J. Hu, J. Hu, W. Hu, W. Huang, W. Hulsbergen, T. Humair, R. J. Hunter, M. Hushchyn, D. Hutchcroft, D. Hynds, P. Ibis, M. Idzik, D. Ilin, P. Ilten, A. Inglessi, K. Ivshin, R. Jacobsson, S. Jakobsen, E. Jans, B. K. Jashal, A. Jawahery, V. Jevtic, F. Jiang, M. John, D. Johnson, C. R. Jones, T. P. Jones, B. Jost, N. Jurik, S. Kandybei, Y. Kang, M. Karacson, J. M. Kariuki, N. Kazeev, M. Kecke, F. Keizer, M. Kelsey, M. Kenzie, T. Ketel, B. Khanji, A. Kharisova, K. E. Kim, 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, O. Lantwin, T. Latham, F. Lazzari, R. Le Gac, S. H. Lee, R. Lefèvre, A. Leflat, O. Leroy, T. Lesiak, B. Leverington, H. Li, L. Li, P. Li, X. 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. Loustau, 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, S. Maccolini, F. Machefert, F. Maciuc, V. Macko, P. Mackowiak, S. Maddrell-Mander, L. R. Madhan Mohan, O. Maev, A. Maevskiy, D. Maisuzenko, M. W. Majewski, S. Malde, B. Malecki, A. Malinin, T. Maltsev, H. Malygina, G. Manca, G. Mancinelli, R. Manera Escalero, D. Manuzzi, D. Marangotto, J. Maratas, J. F. Marchand, U. Marconi, S. Mariani, C. Marin Benito, M. Marinangeli, P. Marino, J. Marks, P. J. Marshall, G. Martellotti, L. Martinazzoli, M. Martinelli, D. Martinez Santos, F. Martinez Vidal, A. Massafferri, M. Materok, R. Matev, A. Mathad, Z. Mathe, V. Matiunin, C. Matteuzzi, K. R. Mattioli, A. Mauri, E. Maurice, M. Mazurek, M. McCann, L. Mcconnell, T. H. Mcgrath, A. McNab, R. McNulty, J. V. Mead, B. Meadows, C. Meaux, G. Meier, N. Meinert, D. Melnychuk, S. Meloni, M. Merk, A. Merli, L. Meyer Garcia, M. Mikhasenko, D. A. Milanes, E. Millard, M.-N. Minard, O. Mineev, L. Minzoni, S. E. Mitchell, B. Mitreska, D. S. Mitzel, A. Mödden, R. A. Mohammed, R. D. Moise, T. Mombächer, I. A. Monroy, S. Monteil, M. Morandin, G. Morello, M. J. Morello, J. Moron, A. B. Morris, A. G. Morris, R. Mountain, H. Mu, F. Muheim, M. Mukherjee, M. Mulder, D. Müller, K. Müller, C. H. Murphy, D. Murray, P. Muzzetto, P. Naik, T. Nakada, R. Nandakumar, T. Nanut, I. Nasteva, M. Needham, I. Neri, N. Neri, S. Neubert, N. Neufeld, R. Newcombe, T. D. Nguyen, C. Nguyen-Mau, E. M. Niel, S. Nieswand, N. Nikitin, N. S. Nolte, C. Nunez, A. Oblakowska-Mucha, V. Obraztsov, S. Ogilvy, D. P. O’Hanlon, R. Oldeman, C. J. G. Onderwater, J. D. Osborn, A. Ossowska, J. M. Otalora Goicochea, T. Ovsiannikova, P. Owen, A. Oyanguren, B. Pagare, P. R. Pais, T. Pajero, A. Palano, M. Palutan, Y. Pan, G. Panshin, A. Papanestis, M. Pappagallo, L. L. Pappalardo, C. Pappenheimer, W. Parker, C. Parkes, C. J. Parkinson, G. Passaleva, A. Pastore, M. Patel, C. Patrignani, A. Pearce, A. Pellegrino, M. Pepe Altarelli, S. Perazzini, D. Pereima, P. Perret, K. Petridis, A. Petrolini, A. Petrov, S. Petrucci, M. Petruzzo, A. Philippov, L. Pica, B. Pietrzyk, G. Pietrzyk, M. Pili, D. Pinci, J. Pinzino, F. Pisani, A. Piucci, V. Placinta, S. Playfer, J. Plews, M. Plo Casasus, F. Polci, M. Poli Lener, M. Poliakova, A. Poluektov, N. Polukhina, I. Polyakov, E. Polycarpo, G. J. Pomery, S. Ponce, A. Popov, D. Popov, S. Popov, S. Poslavskii, K. Prasanth, L. Promberger, C. Prouve, V. Pugatch, A. Puig Navarro, H. Pullen, G. Punzi, W. Qian, J. Qin, R. Quagliani, B. Quintana, N. V. Raab, R. I. Rabadan Trejo, B. Rachwal, J. H. 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ABSTRACT

The decays B+→ J/ψπ+π−K+ are studied using a data set corresponding to an integrated luminosity of 9 fb−1 collected with the LHCb detector in proton-proton collisions between 2011 and 2018. Precise measurements of the ratios of branching fractions with the intermediate ψ2(3823), χc1(3872) and ψ(2S) states are reported. The values areBB+→ψ23823K+×Bψ23823→J/ψπ+π−BB+→χc13872K+×Bχc13872→J/ψπ+π−=3.56±0.67±0.11×10−2,BB+→ψ23823K+×Bψ23823→J/ψπ+π−BB+→ψ2SK+×Bψ2S→J/ψπ+π−=1.31±0.25±0.04×10−3,BB+→χc13872K+×Bχc13872→J/ψπ+π−BB+→ψ2SK+×Bψ2S→J/ψπ+π−=3.69±0.07±0.06×10−2,\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {\displaystyle \begin{array}{c}\frac{{\mathcal{B}}_{{\mathrm{B}}^{+}\to {\uppsi}_2(3823){\mathrm{K}}^{+}}\times {\mathcal{B}}_{\uppsi_2(3823)\to \mathrm{J}/{\uppsi \uppi}^{+}{\uppi}^{-}}}{{\mathcal{B}}_{{\mathrm{B}}^{+}\to {\upchi}_{\mathrm{c}1}(3872){\mathrm{K}}^{+}}\times {\mathcal{B}}_{\upchi_{\mathrm{c}1}(3872)\to \mathrm{J}/{\uppsi \uppi}^{+}{\uppi}^{-}}}=\left(3.56\pm 0.67\pm 0.11\right)\times {10}^{-2},\\ {}\frac{{\mathcal{B}}_{{\mathrm{B}}^{+}\to {\uppsi}_2(3823){\mathrm{K}}^{+}}\times {\mathcal{B}}_{\uppsi_2(3823)\to \mathrm{J}/{\uppsi \uppi}^{+}{\uppi}^{-}}}{{\mathcal{B}}_{{\mathrm{B}}^{+}\to \uppsi \left(2\mathrm{S}\right){\mathrm{K}}^{+}}\times {\mathcal{B}}_{\uppsi \left(2\mathrm{S}\right)\to \mathrm{J}/{\uppsi \uppi}^{+}{\uppi}^{-}}}=\left(1.31\pm 0.25\pm 0.04\right)\times {10}^{-3},\\ {}\frac{{\mathcal{B}}_{\mathrm{B}+\to {\upchi}_{\mathrm{c}1}(3872){\mathrm{K}}^{+}}\times {\mathcal{B}}_{\upchi_{\mathrm{c}1}(3872)\to \mathrm{J}/{\uppsi \uppi}^{+}{\uppi}^{-}}}{{\mathcal{B}}_{{\mathrm{B}}^{+}\to \uppsi \left(2\mathrm{S}\right){\mathrm{K}}^{+}}\times {\mathcal{B}}_{\uppsi \left(2\mathrm{S}\right)\to \mathrm{J}/{\uppsi \uppi}^{+}{\uppi}^{-}}}=\left(3.69\pm 0.07\pm 0.06\right)\times {10}^{-2},\end{array}} $$\end{document}where the first uncertainty is statistical and the second is systematic. The decay of B+→ ψ2(3823)K+ with ψ2(3823) → J/ψπ+π− is observed for the first time with a significance of 5.1 standard deviations. The mass differences between the ψ2(3823), χc1(3872) and ψ(2S) states are measured to bemχc13872−mψ23823=47.50±0.53±0.13MeV/c2,mψ23823−mψ22S=137.98±0.53±0.14MeV/c2,mχc13872−mψ22S=185.49±0.06±0.03MeV/c2,\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {\displaystyle \begin{array}{c}{m}_{\upchi_{\mathrm{c}1}(3872)}-{m}_{\uppsi_2(3823)}=47.50\pm 0.53\pm 0.13\;\mathrm{MeV}/{c}^2,\\ {}{m}_{\uppsi_2(3823)}-{m}_{\uppsi_2\left(2\mathrm{S}\right)}=137.98\pm 0.53\pm 0.14\;\mathrm{MeV}/{c}^2,\\ {}{m}_{\upchi_{\mathrm{c}1}(3872)}-{m}_{\uppsi_2\left(2\mathrm{S}\right)}=185.49\pm 0.06\pm 0.03\;\mathrm{MeV}/{c}^2,\end{array}} $$\end{document}resulting in the most precise determination of the χc1(3872) mass. The width of the ψ2(3823) state is found to be below 5.2 MeV at 90% confidence level. The Breit-Wigner width of the χc1(3872) state is measured to beΓχc13872BW=0.96−0.18+0.19±0.21MeV\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {\Gamma}_{\upchi_{\mathrm{c}1}(3872)}^{\mathrm{BW}}={0.96}_{-0.18}^{+0.19}\pm 0.21\;\mathrm{MeV} $$\end{document}which is inconsistent with zero by 5.5 standard deviations. More... »

PAGES

123

References to SciGraph publications

Journal

TITLE

Journal of High Energy Physics

ISSUE

8

VOLUME

2020

Author Affiliations

  • Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
  • Physik-Institut, Universität Zürich, Zürich, Switzerland
  • Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
  • 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, United Kingdom
  • 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, United Kingdom
  • ICCUB, Universitat de Barcelona, Barcelona, Spain
  • Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
  • Petersburg Nuclear Physics Institute NRC Kurchatov Institute (PNPI NRC KI), Gatchina, Russia
  • 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
  • Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
  • 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
  • Department of Physics, University of Warwick, Coventry, United Kingdom
  • Imperial College London, London, United Kingdom
  • Laboratoire Leprince-Ringuet, Palaiseau, France
  • Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
  • Università 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
  • National Center for Nuclear Research (NCBJ), Warsaw, Poland
  • INFN Sezione di Cagliari, Monserrato, Italy
  • 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
  • Institute of Nuclear Physics, Moscow State University (SINP MSU), Moscow, Russia
  • INFN Sezione di Padova, Padova, Italy
  • Università di Bologna, Bologna, Italy
  • Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
  • 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, United Kingdom
  • Università di Modena e Reggio Emilia, Modena, Italy
  • Department of Physics, University of Oxford, Oxford, United Kingdom
  • INFN Sezione di Roma La Sapienza, Roma, Italy
  • Massachusetts Institute of Technology, Cambridge, MA, United States
  • National Research University Higher School of Economics, Moscow, Russia
  • Novosibirsk State University, Novosibirsk, Russia
  • University of Maryland, College Park, MD, United States
  • 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
  • INFN Sezione di Roma Tor Vergata, Roma, Italy
  • Institute Of High Energy Physics (IHEP), Beijing, China
  • Univ. Grenoble Alpes, Univ. Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France
  • Center for High Energy Physics, Tsinghua University, Beijing, China
  • INFN Sezione di Bologna, Bologna, Italy
  • School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
  • Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest-Magurele, Romania
  • Los Alamos National Laboratory (LANL), Los Alamos, United States
  • Universidad Nacional Autonoma de Honduras, Tegucigalpa, Honduras
  • Università di Bari, Bari, Italy
  • Universiteit Maastricht, Maastricht, Netherlands
  • AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
  • Università di Cagliari, Cagliari, Italy
  • Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
  • Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine
  • School of Physics, University College Dublin, Dublin, Ireland
  • INFN Sezione di Trieste, Trieste, Italy
  • NSC Kharkiv Institute of Physics and Technology (NSC KIPT), Kharkiv, Ukraine
  • STFC Rutherford Appleton Laboratory, Didcot, United Kingdom
  • School of Physics and Astronomy, Monash University, Melbourne, Australia
  • INFN Sezione di Bari, Bari, Italy
  • Università degli Studi di Milano, Milano, Italy
  • School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
  • Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia – CSIC, Valencia, Spain
  • Pontifícia Universidade Católica do Rio de Janeiro (PUC-Rio), Rio de Janeiro, Brazil
  • Universidade Federal do Triângulo Mineiro (UFTM), Uberaba, MG, Brazil
  • Laboratory of Mathematical and Subatomic Physics, Constantine, Algeria
  • Guangdong Provencial Key Laboratory of Nuclear Science, Institute of Quantum Matter, South China Normal University, Guangzhou, China
  • 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
  • MSU - Iligan Institute of Technology (MSU-IIT), Iligan, Philippines
  • INFN Sezione di Milano-Bicocca, Milano, 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
  • Van Swinderen Institute, University of Groningen, Groningen, Netherlands
  • P.N. Lebedev Physical Institute, Russian Academy of Science (LPI RAS), Moscow, Russia
  • Università di Pisa, Pisa, Italy
  • Università di Roma Tor Vergata, Roma, Italy
  • Università della Basilicata, Potenza, Italy
  • Max-Planck-Institut für Kernphysik (MPIK), Heidelberg, Germany
  • Università di Urbino, Urbino, Italy
  • Identifiers

    URI

    http://scigraph.springernature.com/pub.10.1007/jhep08(2020)123

    DOI

    http://dx.doi.org/10.1007/jhep08(2020)123

    DIMENSIONS

    https://app.dimensions.ai/details/publication/pub.1130450494


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        "description": "The decays B+\u2192 J/\u03c8\u03c0+\u03c0\u2212K+ are studied using a data set corresponding to an integrated luminosity of 9 fb\u22121 collected with the LHCb detector in proton-proton collisions between 2011 and 2018. Precise measurements of the ratios of branching fractions with the intermediate \u03c82(3823), \u03c7c1(3872) and \u03c8(2S) states are reported. The values areBB+\u2192\u03c823823K+\u00d7B\u03c823823\u2192J/\u03c8\u03c0+\u03c0\u2212BB+\u2192\u03c7c13872K+\u00d7B\u03c7c13872\u2192J/\u03c8\u03c0+\u03c0\u2212=3.56\u00b10.67\u00b10.11\u00d710\u22122,BB+\u2192\u03c823823K+\u00d7B\u03c823823\u2192J/\u03c8\u03c0+\u03c0\u2212BB+\u2192\u03c82SK+\u00d7B\u03c82S\u2192J/\u03c8\u03c0+\u03c0\u2212=1.31\u00b10.25\u00b10.04\u00d710\u22123,BB+\u2192\u03c7c13872K+\u00d7B\u03c7c13872\u2192J/\u03c8\u03c0+\u03c0\u2212BB+\u2192\u03c82SK+\u00d7B\u03c82S\u2192J/\u03c8\u03c0+\u03c0\u2212=3.69\u00b10.07\u00b10.06\u00d710\u22122,\\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}$$ {\\displaystyle \\begin{array}{c}\\frac{{\\mathcal{B}}_{{\\mathrm{B}}^{+}\\to {\\uppsi}_2(3823){\\mathrm{K}}^{+}}\\times {\\mathcal{B}}_{\\uppsi_2(3823)\\to \\mathrm{J}/{\\uppsi \\uppi}^{+}{\\uppi}^{-}}}{{\\mathcal{B}}_{{\\mathrm{B}}^{+}\\to {\\upchi}_{\\mathrm{c}1}(3872){\\mathrm{K}}^{+}}\\times {\\mathcal{B}}_{\\upchi_{\\mathrm{c}1}(3872)\\to \\mathrm{J}/{\\uppsi \\uppi}^{+}{\\uppi}^{-}}}=\\left(3.56\\pm 0.67\\pm 0.11\\right)\\times {10}^{-2},\\\\ {}\\frac{{\\mathcal{B}}_{{\\mathrm{B}}^{+}\\to {\\uppsi}_2(3823){\\mathrm{K}}^{+}}\\times {\\mathcal{B}}_{\\uppsi_2(3823)\\to \\mathrm{J}/{\\uppsi \\uppi}^{+}{\\uppi}^{-}}}{{\\mathcal{B}}_{{\\mathrm{B}}^{+}\\to \\uppsi \\left(2\\mathrm{S}\\right){\\mathrm{K}}^{+}}\\times {\\mathcal{B}}_{\\uppsi \\left(2\\mathrm{S}\\right)\\to \\mathrm{J}/{\\uppsi \\uppi}^{+}{\\uppi}^{-}}}=\\left(1.31\\pm 0.25\\pm 0.04\\right)\\times {10}^{-3},\\\\ {}\\frac{{\\mathcal{B}}_{\\mathrm{B}+\\to {\\upchi}_{\\mathrm{c}1}(3872){\\mathrm{K}}^{+}}\\times {\\mathcal{B}}_{\\upchi_{\\mathrm{c}1}(3872)\\to \\mathrm{J}/{\\uppsi \\uppi}^{+}{\\uppi}^{-}}}{{\\mathcal{B}}_{{\\mathrm{B}}^{+}\\to \\uppsi \\left(2\\mathrm{S}\\right){\\mathrm{K}}^{+}}\\times {\\mathcal{B}}_{\\uppsi \\left(2\\mathrm{S}\\right)\\to \\mathrm{J}/{\\uppsi \\uppi}^{+}{\\uppi}^{-}}}=\\left(3.69\\pm 0.07\\pm 0.06\\right)\\times {10}^{-2},\\end{array}} $$\\end{document}where the first uncertainty is statistical and the second is systematic. The decay of B+\u2192 \u03c82(3823)K+ with \u03c82(3823) \u2192 J/\u03c8\u03c0+\u03c0\u2212 is observed for the first time with a significance of 5.1 standard deviations. The mass differences between the \u03c82(3823), \u03c7c1(3872) and \u03c8(2S) states are measured to bem\u03c7c13872\u2212m\u03c823823=47.50\u00b10.53\u00b10.13MeV/c2,m\u03c823823\u2212m\u03c822S=137.98\u00b10.53\u00b10.14MeV/c2,m\u03c7c13872\u2212m\u03c822S=185.49\u00b10.06\u00b10.03MeV/c2,\\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}$$ {\\displaystyle \\begin{array}{c}{m}_{\\upchi_{\\mathrm{c}1}(3872)}-{m}_{\\uppsi_2(3823)}=47.50\\pm 0.53\\pm 0.13\\;\\mathrm{MeV}/{c}^2,\\\\ {}{m}_{\\uppsi_2(3823)}-{m}_{\\uppsi_2\\left(2\\mathrm{S}\\right)}=137.98\\pm 0.53\\pm 0.14\\;\\mathrm{MeV}/{c}^2,\\\\ {}{m}_{\\upchi_{\\mathrm{c}1}(3872)}-{m}_{\\uppsi_2\\left(2\\mathrm{S}\\right)}=185.49\\pm 0.06\\pm 0.03\\;\\mathrm{MeV}/{c}^2,\\end{array}} $$\\end{document}resulting in the most precise determination of the \u03c7c1(3872) mass. The width of the \u03c82(3823) state is found to be below 5.2 MeV at 90% confidence level. The Breit-Wigner width of the \u03c7c1(3872) state is measured to be\u0393\u03c7c13872BW=0.96\u22120.18+0.19\u00b10.21MeV\\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}$$ {\\Gamma}_{\\upchi_{\\mathrm{c}1}(3872)}^{\\mathrm{BW}}={0.96}_{-0.18}^{+0.19}\\pm 0.21\\;\\mathrm{MeV} $$\\end{document}which is inconsistent with zero by 5.5 standard deviations.", 
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    10 schema:description The decays B+→ J/ψπ+π−K+ are studied using a data set corresponding to an integrated luminosity of 9 fb−1 collected with the LHCb detector in proton-proton collisions between 2011 and 2018. Precise measurements of the ratios of branching fractions with the intermediate ψ2(3823), χc1(3872) and ψ(2S) states are reported. The values areBB+→ψ23823K+×Bψ23823→J/ψπ+π−BB+→χc13872K+×Bχc13872→J/ψπ+π−=3.56±0.67±0.11×10−2,BB+→ψ23823K+×Bψ23823→J/ψπ+π−BB+→ψ2SK+×Bψ2S→J/ψπ+π−=1.31±0.25±0.04×10−3,BB+→χc13872K+×Bχc13872→J/ψπ+π−BB+→ψ2SK+×Bψ2S→J/ψπ+π−=3.69±0.07±0.06×10−2,\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {\displaystyle \begin{array}{c}\frac{{\mathcal{B}}_{{\mathrm{B}}^{+}\to {\uppsi}_2(3823){\mathrm{K}}^{+}}\times {\mathcal{B}}_{\uppsi_2(3823)\to \mathrm{J}/{\uppsi \uppi}^{+}{\uppi}^{-}}}{{\mathcal{B}}_{{\mathrm{B}}^{+}\to {\upchi}_{\mathrm{c}1}(3872){\mathrm{K}}^{+}}\times {\mathcal{B}}_{\upchi_{\mathrm{c}1}(3872)\to \mathrm{J}/{\uppsi \uppi}^{+}{\uppi}^{-}}}=\left(3.56\pm 0.67\pm 0.11\right)\times {10}^{-2},\\ {}\frac{{\mathcal{B}}_{{\mathrm{B}}^{+}\to {\uppsi}_2(3823){\mathrm{K}}^{+}}\times {\mathcal{B}}_{\uppsi_2(3823)\to \mathrm{J}/{\uppsi \uppi}^{+}{\uppi}^{-}}}{{\mathcal{B}}_{{\mathrm{B}}^{+}\to \uppsi \left(2\mathrm{S}\right){\mathrm{K}}^{+}}\times {\mathcal{B}}_{\uppsi \left(2\mathrm{S}\right)\to \mathrm{J}/{\uppsi \uppi}^{+}{\uppi}^{-}}}=\left(1.31\pm 0.25\pm 0.04\right)\times {10}^{-3},\\ {}\frac{{\mathcal{B}}_{\mathrm{B}+\to {\upchi}_{\mathrm{c}1}(3872){\mathrm{K}}^{+}}\times {\mathcal{B}}_{\upchi_{\mathrm{c}1}(3872)\to \mathrm{J}/{\uppsi \uppi}^{+}{\uppi}^{-}}}{{\mathcal{B}}_{{\mathrm{B}}^{+}\to \uppsi \left(2\mathrm{S}\right){\mathrm{K}}^{+}}\times {\mathcal{B}}_{\uppsi \left(2\mathrm{S}\right)\to \mathrm{J}/{\uppsi \uppi}^{+}{\uppi}^{-}}}=\left(3.69\pm 0.07\pm 0.06\right)\times {10}^{-2},\end{array}} $$\end{document}where the first uncertainty is statistical and the second is systematic. The decay of B+→ ψ2(3823)K+ with ψ2(3823) → J/ψπ+π− is observed for the first time with a significance of 5.1 standard deviations. The mass differences between the ψ2(3823), χc1(3872) and ψ(2S) states are measured to bemχc13872−mψ23823=47.50±0.53±0.13MeV/c2,mψ23823−mψ22S=137.98±0.53±0.14MeV/c2,mχc13872−mψ22S=185.49±0.06±0.03MeV/c2,\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {\displaystyle \begin{array}{c}{m}_{\upchi_{\mathrm{c}1}(3872)}-{m}_{\uppsi_2(3823)}=47.50\pm 0.53\pm 0.13\;\mathrm{MeV}/{c}^2,\\ {}{m}_{\uppsi_2(3823)}-{m}_{\uppsi_2\left(2\mathrm{S}\right)}=137.98\pm 0.53\pm 0.14\;\mathrm{MeV}/{c}^2,\\ {}{m}_{\upchi_{\mathrm{c}1}(3872)}-{m}_{\uppsi_2\left(2\mathrm{S}\right)}=185.49\pm 0.06\pm 0.03\;\mathrm{MeV}/{c}^2,\end{array}} $$\end{document}resulting in the most precise determination of the χc1(3872) mass. The width of the ψ2(3823) state is found to be below 5.2 MeV at 90% confidence level. The Breit-Wigner width of the χc1(3872) state is measured to beΓχc13872BW=0.96−0.18+0.19±0.21MeV\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {\Gamma}_{\upchi_{\mathrm{c}1}(3872)}^{\mathrm{BW}}={0.96}_{-0.18}^{+0.19}\pm 0.21\;\mathrm{MeV} $$\end{document}which is inconsistent with zero by 5.5 standard deviations.
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