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Observation of the decay Λb 0→Λc +pp‾π

  • LHCb Collaboration
  • Science Park 105
  • Universidade de Santiago de Compostela
  • University of Bristol
  • Clermont-Auvergne University
  • University of Cincinnati
  • LNF-INFN
  • University of Dortmund
  • European Organization for Nuclear Research
  • University of Glasgow
  • University of Barcelona
  • Petersburg Nuclear Physics Institute (PNPI)
  • Imperial College London
  • Instituto de Biofisica da UFRJ
  • INFN
  • Laboratoire de l'Accélérateur Linéaire
  • Tsinghua University
  • Istituto Nazionale di Fisica Nucleare, Sezione di Firenze
  • ENAC-IIC-GEL
  • Sezione INFN di Ferrara
  • University of Ferrara
  • University of Maryland, College Park
  • University of Manchester
  • University of Heidelberg
  • Aix Marseille Université
  • Kurchatov Institute
  • Syracuse University
  • University of Zurich
  • Sezione di Roma
  • University of Warwick
  • Yandex School of Data Analysis
  • Institute for Theoretical and Experimental Physics
  • National Centre for Nuclear Research (NCBJ)
  • Istituto Nazionale di Fisica Nucleare, Sezione di Pisa
  • Centro Brasileiro de Pesquisas Fisicas
  • University of Chinese Academy of Sciences
  • INFN Sezione di Milano-Bicocca
  • University of Milano-Bicocca
  • Universités Paris VI and VII
  • RWTH Aachen University
  • Moscow State University
  • INFN Sezione di Bologna
  • University of Cambridge
  • University of Birmingham
  • University of Modena and Reggio Emilia
  • University of Oxford
  • Massachusetts Institute of Technology
  • Budker Institute of Nuclear Physics of the Siberian Branch of the RAS
  • Novosibirsk State University
  • University of Liverpool
  • Institute for Nuclear Physics
  • Sezione INFN di Cagliari
  • Wuhan University
  • Universitat Ramon LLull - CSIC
  • University of Bologna
  • Sezione di Genova
  • University of Genoa
  • University of Edinburgh
  • University of Pisa
  • LTHE (UMR 5564 CNRS/IRD/Université de Grenoble)
  • Universitá di Cagliari
  • Horia Hulubei National Institute of Physics and Nuclear Engineering
  • MST-8, Los Alamos National Laboratory
  • INFN Sezione di Bari
  • Università degli studi di Bari Aldo Moro
  • Max-Planck-Institut für Kernphysik
  • Agh University of Science and Technology Faculty of Computer Science
  • Central China Normal University
  • National University of Science and Technology “MISIS”
  • Kharkov Institute of Physics and Technology
  • CCLRC Rutherford Appleton Laboratory
  • Institute for Nuclear Research of the Russian Academy of Sciences
  • Sezione INFN di Milano
  • University of Milano
  • University of Valencia
  • Universidade Federal Do Triângulo Mineiro (UFTM)
  • Universität Rostock
  • Pontifícia Universidade Católica do Rio de Janeiro
  • Vrije Universiteit Amsterdam
  • Institute of Nuclear Research, National Academy of Sciences in Ukraine
  • Kurchatov Institute
  • University of Padova
  • Iligan Institute of Technology (IIT)
  • University College Dublin
  • Universidad Nacional de Colombia
  • Escuela Agrícola Panamericana
  • Scuola Normale Superiore di Pisa
  • Hanoi University of Science
  • ICS/University of Groningen
  • National Research Tomsk Polytechnic University
  • National Research University
  • University of Rome “Tor Vergata”
  • University of Rome
  • Università degli Studi della Basilicata
  • University of Urbino Carlo Bo
  • P.N. Lebedev Physical Institute of the Russian Academy of Sciences

Résultats de recherche: Contribution à un journalArticleRevue par des pairs

Résumé

The decay Λb 0→Λc +pp‾π is observed using pp collision data collected with the LHCb detector at centre-of-mass energies of s=7 and 8 Tev, corresponding to an integrated luminosity of 3 fb−1. The ratio of branching fractions between Λb 0→Λc +pp‾π and Λb 0→Λc +π decays is measured to be [Formula presented]=0.0540±0.0023±0.0032. Two resonant structures are observed in the Λc +π mass spectrum of the Λb 0→Λc +pp‾π decays, corresponding to the Σc(2455)0 and Σc (2520)0 states. The ratios of branching fractions with respect to the decay Λb 0→Λc +pp‾π are [Formula presented]=0.089±0.015±0.006,[Formula presented]=0.119±0.020±0.014. In all of the above results, the first uncertainty is statistical and the second is systematic. The phase space is also examined for the presence of dibaryon resonances. No evidence for such resonances is found.

langue originaleAnglais
Pages (de - à)101-111
Nombre de pages11
journalPhysics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics
Volume784
Les DOIs
étatPublié - 10 sept. 2018

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