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D-meson production in p-Pb collisions at s NN =5.02 TeV and in pp collisions at s =7 TeV

  • ALICE Collaboration
  • Czech Technical University in Prague
  • Czech Academy of Sciences
  • Panjab University
  • CERN
  • Politecnico di Torino
  • Sezione INFN
  • Indian Institute of Technology Bombay
  • Variable Energy Cyclotron Centre
  • Aligarh Muslim University
  • Korea Institute of Science and Technology Information
  • Yale University
  • Alikhanov Institute for Theoretical and Experimental Physics
  • Universidade Estadual de Campinas
  • Russian Research Centre Kurchatov Institute
  • University of Birmingham
  • Universidad Nacional Autónoma de México
  • Centro Fermi - Museo Storico della Fisica e Centro Studi e Ricerche Enrico Fermi
  • National Institute for Nuclear Physics
  • Bogolyubov Institute for Theoretical Physics Nasu
  • University of Bergen
  • Western Norway University of Applied Sciences
  • Frankfurt Institute for Advanced Studies
  • St. Petersburg State University
  • Universidade de São Paulo
  • National Institute for Physics and Nuclear Engineering
  • GSI Helmholtzzentrum für Schwerionenforschung
  • Ruprecht-Karls-Universität Heidelberg
  • Ruder Boskovic Institute
  • Nantes Université
  • Goethe University Frankfurt
  • University of Bologna
  • Technische Universität München
  • Technical University of Munich
  • University of Oslo
  • Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN
  • Konkuk University
  • University of Jammu
  • IRFU
  • Institute of Physics Bhubaneswar
  • University of Catania
  • Hungarian Academy of Sciences
  • Université Clermont Auvergne
  • Central China Normal University
  • Henryk Niewodniczanski Institute of Nuclear Physics of the Polish Academy of Sciences
  • M.V.Lomonosov Moscow State University
  • University of Münster
  • Joint Institute for Nuclear Research
  • University of Copenhagen
  • Inha University
  • Université de Strasbourg
  • Benemérita Universidad Autónoma de Puebla
  • University of Houston
  • Wayne State University
  • Universidad Autonoma de Sinaloa
  • Moscow Engineering Physics Institute
  • Petersburg Nuclear Physics Institute (PNPI)
  • Institute for Subatomic Physics of Utrecht University
  • Gauhati University
  • INFN, Laboratori Nazionali Di Frascati
  • Bose Institute
  • National Institute of Science Education and Research
  • University of Texas at Austin
  • Lawrence Berkeley National Laboratory
  • Pavol Jozef Šafárik University
  • Pusan National University
  • STFC Daresbury Laboratory
  • University of Liverpool
  • National Research Foundation
  • Purdue University
  • University of Helsinki
  • Russian Federal Nuclear Center (VNIIEF)
  • University of Tsukuba
  • COMSATS University Islamabad
  • Ohio State University
  • Technical University of Košice
  • Pontifical Catholic Univ. of Peru
  • University of Tennessee
  • Sezione INFN
  • Centro de Aplicaciones Tecnológicas y Desarrollo Nuclear
  • University of Jyväskylä
  • Saha Institute of Nuclear Physics
  • Creighton University
  • Universite Claude Bernard Lyon 1
  • National Institute for Subatomic Physics
  • University of Lund
  • University of Cape Town
  • Slovak Academy of Sciences
  • Université Grenoble Alpes
  • CNRS-IN2P3
  • Georgia State University
  • Oak Ridge National Laboratory
  • Centro de Investigación y de Estudios AVanzados (CINVESTAV)
  • Institute of Space Science (ISS)
  • National Centre for Nuclear Studies
  • Centro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT)
  • University of Zagreb
  • Institute for High Energy Physics
  • Universidad de Santiago de Compostela
  • RAS - Institute for Nuclear Research
  • National and Kapodistrian University of Athens
  • Chicago State University
  • University of Split
  • Warsaw University of Technology
  • A. Alikhanian Yerevan Institute of Physics
  • Austrian Academy of Sciences
  • Tokyo University
  • Eberhard Karls Universität Tübingen
  • Sejong University
  • Yonsei University
  • KTO Karatay University
  • Fachhochschule Worms
  • Gangneung-Wonju National University
  • California Polytechnic State University, San Luis Obispo
  • Suranaree University of Technology
  • University of South-Eastern Norway
  • China Institute of Atomic Energy
  • University of the Witwatersrand
  • Institute of Physics of the Czech Academy of Sciences
  • University of Rome La Sapienza
  • Comenius University
  • Indian Institute of Technology Indore
  • Rheinische Friedrich-Wilhelms-Universität Bonn
  • Hiroshima University
  • Nagasaki Institute of Applied Science
  • Università di Brescia
  • Budker Institute for Nuclear Physics
  • University of Rajasthan
  • Laboratori Nazionali di Legnaro
  • Indonesian Institute of Sciences
  • Centre de calcul de l'IN2P3

Research output: Contribution to journalArticlepeer-review

101 Scopus citations

Abstract

Background: In the context of the investigation of the quark gluon plasma produced in heavy-ion collisions, hadrons containing heavy (charm or beauty) quarks play a special role for the characterization of the hot and dense medium created in the interaction. The measurement of the production of charm and beauty hadrons in proton-proton collisions, besides providing the necessary reference for the studies in heavy-ion reactions, constitutes an important test of perturbative quantum chromodynamics (pQCD) calculations. Heavy-flavor production in proton-nucleus collisions is sensitive to the various effects related to the presence of nuclei in the colliding system, commonly denoted cold-nuclear-matter effects. Most of these effects are expected to modify open-charm production at low transverse momenta (pT) and, so far, no measurement of D-meson production down to zero transverse momentum was available at mid-rapidity at the energies attained at the CERN Large Hadron Collider (LHC). Purpose: The measurements of the production cross sections of promptly produced charmed mesons in p-Pb collisions at the LHC down to pT=0 and the comparison to the results from pp interactions are aimed at the assessment of cold-nuclear-matter effects on open-charm production, which is crucial for the interpretation of the results from Pb-Pb collisions. Methods: The prompt charmed mesons D0,D+,D∗+, and Ds+ were measured at mid-rapidity in p-Pb collisions at a center-of-mass energy per nucleon pair sNN=5.02 TeV with the ALICE detector at the LHC. D mesons were reconstructed from their decays D0→K-π+,D+→K-π+π+, D∗+→D0π+,Ds+→φπ+→K-K+π+, and their charge conjugates, using an analysis method based on the selection of decay topologies displaced from the interaction vertex. In addition, the prompt D0 production cross section was measured in pp collisions at s=7 TeV and p-Pb collisions at sNN=5.02 TeV down to pT=0 using an analysis technique that is based on the estimation and subtraction of the combinatorial background, without reconstruction of the D0 decay vertex. Results: The production cross section in pp collisions is described within uncertainties by different implementations of pQCD calculations down to pT=0. This allowed also a determination of the total cc production cross section in pp collisions, which is more precise than previous ALICE measurements because it is not affected by uncertainties owing to the extrapolation to pT=0. The nuclear modification factor RpPb(pT), defined as the ratio of the pT-differential D meson cross section in p-Pb collisions and that in pp collisions scaled by the mass number of the Pb nucleus, was calculated for the four D-meson species and found to be compatible with unity within uncertainties. The results are compared to theoretical calculations that include cold-nuclear-matter effects and to transport model calculations incorporating the interactions of charm quarks with an expanding deconfined medium. Conclusions: These measurements add experimental evidence that the modification of the D-meson transverse momentum distributions observed in Pb-Pb collisions with respect to pp interactions is due to strong final-state effects induced by the interactions of the charm quarks with the hot and dense partonic medium created in ultrarelativistic heavy-ion collisions. The current precision of the measurement does not allow us to draw conclusions on the role of the different cold-nuclear-matter effects and on the possible presence of additional hot-medium effects in p-Pb collisions. However, the analysis technique without decay-vertex reconstruction, applied on future larger data samples, should provide access to the physics-rich range down to pT=0.

Original languageEnglish
Article number054908
JournalPhysical Review C
Volume94
Issue number5
DOIs
StatePublished - 23 Nov 2016

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