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Light neutral-meson production in pp collisions at = 13 TeV

  • The ALICE collaboration
  • CERN
  • Université Clermont Auvergne
  • Variable Energy Cyclotron Centre
  • Sezione INFN
  • National Institute for Nuclear Physics
  • Department of Physics Aligarh Muslim University
  • Korea Institute of Science and Technology Information
  • Pavol Jozef Šafárik University
  • Frankfurt Institute for Advanced Studies
  • GSI Helmholtzzentrum für Schwerionenforschung
  • Central China Normal University
  • Universidad Nacional Autónoma de México
  • University of Houston
  • Sungkyunkwan University
  • University of Bergen
  • Goethe University Frankfurt
  • Sezione INFN
  • Technical University of Munich
  • Benemérita Universidad Autónoma de Puebla
  • National Institute for Physics and Nuclear Engineering
  • University of Derby
  • University of Münster
  • Ruprecht-Karls-Universität Heidelberg
  • Lawrence Berkeley National Laboratory
  • Nantes Université
  • Université Grenoble Alpes
  • Universidade de São Paulo
  • University of Oslo
  • Yale University
  • Tokyo University
  • Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN
  • Gangneung-Wonju National University
  • University of Science and Technology of China
  • Indian Institute of Technology Indore
  • University of Jammu
  • CNRS-IN2P3
  • AGH University of Krakow
  • National and Kapodistrian University of Athens
  • Gauhati University
  • Wigner Research Centre for Physics
  • University of Liverpool
  • University of Lund
  • Indian Institute of Technology Bombay
  • University of Copenhagen
  • Université de Strasbourg
  • Universidad Autonoma de Sinaloa
  • Institute of Space Science (ISS)
  • Czech Technical University in Prague
  • Czech Academy of Sciences
  • University of Kansas
  • Bose Institute
  • University of Texas at Austin
  • Oak Ridge National Laboratory
  • Pusan National University
  • Università di Brescia
  • Polytechnic University of Bari
  • Sofia University St. Kliment Ohridski
  • STFC Daresbury Laboratory
  • Austrian Academy of Sciences
  • National Research Foundation
  • University of the Witwatersrand
  • Henryk Niewodniczanski Institute of Nuclear Physics of the Polish Academy of Sciences
  • Pontifical Catholic Univ. of Peru
  • National University of Science and Technology POLITEHNICA Bucharest
  • Warsaw University of Technology
  • Fudan University
  • Université de Lyon
  • Max-Planck-Institut für Physik
  • Inha University
  • Homi Bhabha National Institute
  • National Institute for Subatomic Physics
  • University of Tsukuba
  • Agenzia nazionale per le nuove tecnologie, l'energia e lo sviluppo economico sostenibile
  • University of Birmingham
  • Università del Piemonte Orientale and Gruppo Collegato INFN
  • Universidade Federal do ABC
  • University of Pavia
  • University of California at Berkeley
  • Università degli Studi di Foggia
  • Centro de Aplicaciones Tecnológicas y Desarrollo Nuclear
  • Comenius University
  • Hiroshima University
  • INFN, Laboratori Nazionali Di Frascati
  • Politecnico di Torino
  • Saga University
  • Chicago State University
  • Universidade Federal do Rio Grande do Sul
  • University of Tennessee
  • Nagasaki Institute of Applied Science
  • Wayne State University
  • University of Split
  • Institute for Subatomic Physics of Utrecht University
  • A. I. Alikhanyan National Science Laboratory (YereVan Physics Institute) Foundation
  • Universidade Estadual de Campinas
  • Yonsei University
  • University of Jyväskylä
  • Rheinische Friedrich-Wilhelms-Universität Bonn
  • Faculty of Technology
  • Centro de Investigación y de Estudios AVanzados (CINVESTAV)
  • Ohio State University
  • Technical University of Košice
  • National Research and Innovation Agency Republic of Indonesia
  • China Institute of Atomic Energy
  • Suranaree University of Technology
  • Slovak Academy of Sciences
  • Yildiz Technical University
  • University of Zagreb
  • Jeonbuk National University
  • Sejong University
  • California Polytechnic State University, San Luis Obispo
  • Panjab University
  • National Centre for Nuclear Studies
  • Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN
  • University of South-Eastern Norway
  • University of Messina
  • University of Helsinki
  • University of Cape Town
  • Chungbuk National University
  • China University of Geosciences
  • Creighton University
  • University of Wrocław
  • National Nuclear Research Center
  • Eberhard Karls Universität Tübingen
  • Nara Women's University
  • Bogolyubov Institute for Theoretical Physics Nasu
  • Institute of Physics of the Czech Academy of Sciences

Research output: Contribution to journalArticlepeer-review

2 Scopus citations

Abstract

The momentum-differential invariant cross sections of π0 and η mesons are reported for pp collisions at = 13 TeV at midrapidity (|y| < 0.8). The measurement is performed in a broad transverse-momentum range of 0.2 < pT< 200 GeV/c and 0.4 < pT< 60 GeV/c for the π0 and η, respectively, extending the pT coverage of previous measurements. Transverse-mass-scaling violation of up to 60% at low transverse momentum has been observed, agreeing with measurements at lower collision energies. Transverse Bjorken x (xT) scaling of the π0 cross sections at LHC energies is fulfilled with a power-law exponent of n = 5.01 ± 0.05, consistent with values obtained for charged pions at similar collision energies. The data are compared to predictions from next-to-leading order perturbative QCD calculations, where the π0 spectrum is best described using the CT18 parton distribution function and the NNFF1.0 or BDSS fragmentation function. Expectations from PYTHIA8 and EPOS LHC overestimate the spectrum for the π0 and are not able to describe the shape and magnitude of the η spectrum. The charged-particle multiplicity dependent π0 and η pT spectra show the expected change of the spectral shape, characterized by a flatter slope with increasing multiplicity. This is demonstrated across a broad transverse-momentum range and up to events with a charged-particle multiplicity exceeding five times the mean value in minimum bias collisions. The η/π0 ratio depends on the charged-particle multiplicity for pT< 4 GeV/c. PYTHIA8 and EPOS LHC qualitatively explain this behavior with an increasing contribution from the feed-down of heavier particles to the π0 spectrum.

Original languageEnglish
Article number35
JournalJournal of High Energy Physics
Volume2025
Issue number8
DOIs
StatePublished - Aug 2025

Keywords

  • Hadron-Hadron Scattering
  • Particle and Resonance Production
  • QCD

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