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Enhanced Production of Λ_{b}
Aaij, R; Abdelmotteleb, A S W; Abellan Beteta, C; Abudinén, F; Ackernley, T; Adeva, B; Adinolfi, M; Adlarson, P; Agapopoulou, C; Aidala, C A; Ajaltouni, Z; Akar, S; Akiba, K; Albicocco, P; Albrecht, J; Alessio, F; Alexander, M; Alfonso Albero, A; Aliouche, Z; Alvarez Cartelle, P; Amalric, R; Amato, S; Amey, J L; Amhis, Y; An, L; Anderlini, L; Andersson, M; Andreianov, A; Andreola, P; Andreotti, M; Andreou, D; Anelli, A A; Ao, D; Archilli, F; Argenton, M; Arguedas Cuendis, S; Artamonov, A; Artuso, M; Aslanides, E; Atzeni, M; Audurier, B; Bacher, D; Bachiller Perea, I; Bachmann, S; Bachmayer, M; Back, J J; Bailly-Reyre, A; Baladron Rodriguez, P; Balagura, V; Baldini, W.
Afiliación
  • Aaij R; Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands.
  • Abdelmotteleb ASW; Department of Physics, University of Warwick, Coventry, United Kingdom.
  • Abellan Beteta C; Physik-Institut, Universität Zürich, Zürich, Switzerland.
  • Abudinén F; Department of Physics, University of Warwick, Coventry, United Kingdom.
  • Ackernley T; Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom.
  • Adeva B; Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain.
  • Adinolfi M; H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom.
  • Adlarson P; Department of Physics and Astronomy, Uppsala University, Uppsala, Sweden (associated with School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom).
  • Agapopoulou C; European Organization for Nuclear Research (CERN), Geneva, Switzerland.
  • Aidala CA; University of Michigan, Ann Arbor, Michigan, USA (associated with Syracuse University, Syracuse, New York, USA).
  • Ajaltouni Z; Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France.
  • Akar S; University of Cincinnati, Cincinnati, Ohio, USA.
  • Akiba K; Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands.
  • Albicocco P; INFN Laboratori Nazionali di Frascati, Frascati, Italy.
  • Albrecht J; Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany.
  • Alessio F; European Organization for Nuclear Research (CERN), Geneva, Switzerland.
  • Alexander M; School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom.
  • Alfonso Albero A; ICCUB, Universitat de Barcelona, Barcelona, Spain.
  • Aliouche Z; Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom.
  • Alvarez Cartelle P; Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom.
  • Amalric R; LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France.
  • Amato S; Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil.
  • Amey JL; H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom.
  • Amhis Y; Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France.
  • An L; European Organization for Nuclear Research (CERN), Geneva, Switzerland.
  • Anderlini L; School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China.
  • Andersson M; INFN Sezione di Firenze, Firenze, Italy.
  • Andreianov A; Physik-Institut, Universität Zürich, Zürich, Switzerland.
  • Andreola P; Affiliated with an institute covered by a cooperation agreement with CERN.
  • Andreotti M; Physik-Institut, Universität Zürich, Zürich, Switzerland.
  • Andreou D; INFN Sezione di Ferrara, Ferrara, Italy.
  • Anelli AA; Syracuse University, Syracuse, New York, USA.
  • Ao D; INFN Sezione di Milano-Bicocca, Milano, Italy.
  • Archilli F; University of Chinese Academy of Sciences, Beijing, China.
  • Argenton M; INFN Sezione di Roma Tor Vergata, Roma, Italy.
  • Arguedas Cuendis S; INFN Sezione di Ferrara, Ferrara, Italy.
  • Artamonov A; Consejo Nacional de Rectores (CONARE), San Jose, Costa Rica.
  • Artuso M; Affiliated with an institute covered by a cooperation agreement with CERN.
  • Aslanides E; Syracuse University, Syracuse, New York, USA.
  • Atzeni M; Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France.
  • Audurier B; Massachusetts Institute of Technology, Cambridge, Massachusetts, USA.
  • Bacher D; Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France.
  • Bachiller Perea I; Department of Physics, University of Oxford, Oxford, United Kingdom.
  • Bachmann S; Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France.
  • Bachmayer M; Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany.
  • Back JJ; Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland.
  • Bailly-Reyre A; Department of Physics, University of Warwick, Coventry, United Kingdom.
  • Baladron Rodriguez P; LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France.
  • Balagura V; Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain.
  • Baldini W; Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France.
Phys Rev Lett ; 132(8): 081901, 2024 Feb 23.
Article en En | MEDLINE | ID: mdl-38457697
ABSTRACT
The production rate of Λ_{b}^{0} baryons relative to B^{0} mesons in pp collisions at a center-of-mass energy sqrt[s]=13 TeV is measured by the LHCb experiment. The ratio of Λ_{b}^{0} to B^{0} production cross sections shows a significant dependence on both the transverse momentum and the measured charged-particle multiplicity. At low multiplicity, the ratio measured at LHCb is consistent with the value measured in e^{+}e^{-} collisions, and increases by a factor of ∼2 with increasing multiplicity. At relatively low transverse momentum, the ratio of Λ_{b}^{0} to B^{0} cross sections is higher than what is measured in e^{+}e^{-} collisions, but converges with the e^{+}e^{-} ratio as the momentum increases. These results imply that the evolution of heavy b quarks into final-state hadrons is influenced by the density of the hadronic environment produced in the collision. Comparisons with several models and implications for the mechanisms enforcing quark confinement are discussed.

Texto completo: 1 Colección: 01-internacional Banco de datos: MEDLINE Idioma: En Revista: Phys Rev Lett Año: 2024 Tipo del documento: Article País de afiliación: Países Bajos

Texto completo: 1 Colección: 01-internacional Banco de datos: MEDLINE Idioma: En Revista: Phys Rev Lett Año: 2024 Tipo del documento: Article País de afiliación: Países Bajos