Production of K S 0 $$ {\textrm{K}}_{\textrm{S}}^0 $$ , Λ ( Λ ¯ $$ \overline{\Lambda} $$ ), Ξ ± , and Ω ± in jets and in the underlying event in pp and p–Pb collisions

S. Acharya (Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France) ; D. Adamová (Nuclear Physics Institute of the Czech Academy of Sciences, Husinec-Řež, Czech Republic) ; A. Adler (Johann-Wolfgang-Goethe Universität Frankfurt Institut für Informatik, Fachbereich Informatik und Mathematik, Frankfurt, Germany) ; G. Aglieri Rinella (European Organization for Nuclear Research (CERN), Geneva, Switzerland) ; M. Agnello (Dipartimento DISAT del Politecnico and Sezione INFN, Turin, Italy) ; et al. - Show all 1032 authors

The production of strange hadrons ( K S 0 $$ {\textrm{K}}_{\textrm{S}}^0 $$ , Λ, Ξ ± , and Ω ± ), baryon-to-meson ratios (Λ/ K S 0 $$ {\textrm{K}}_{\textrm{S}}^0 $$ , Ξ/ K S 0 $$ {\textrm{K}}_{\textrm{S}}^0 $$ , and Ω/ K S 0 $$ {\textrm{K}}_{\textrm{S}}^0 $$ ), and baryon-to-baryon ratios (Ξ/Λ, Ω/Λ, and Ω/Ξ) associated with jets and the underlying event were measured as a function of transverse momentum (p T) in pp collisions at s $$ \sqrt{s} $$ = 13 TeV and p Pb collisions at s NN $$ \sqrt{s_{\textrm{NN}}} $$ = 5.02 TeV with the ALICE detector at the LHC. The inclusive production of the same particle species and the corresponding ratios are also reported. The production of multi-strange hadrons, Ξ ± and Ω ± , and their associated particle ratios in jets and in the underlying event are measured for the first time. In both pp and p–Pb collisions, the baryon-to-meson and baryon-to-baryon yield ratios measured in jets differ from the inclusive particle production for low and intermediate hadron p T (0.6–6 GeV/c). Ratios measured in the underlying event are in turn similar to those measured for inclusive particle production. In pp collisions, the particle production in jets is compared with Pythia 8 predictions with three colour-reconnection implementation modes. None of them fully reproduces the data in the measured hadron p T region. The maximum deviation is observed for Ξ ± and Ω ± which reaches a factor of about six. The event multiplicity dependence is further investigated in p−Pb collisions. In contrast to what is observed in the underlying event, there is no significant event-multiplicity dependence for particle production in jets. The presented measurements provide novel constraints on hadronisation and its Monte Carlo description. In particular, they demonstrate that the fragmentation of jets alone is insufficient to describe the strange and multi-strange particle production in hadronic collisions at LHC energies.

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    "updated": "2023-10-24T00:35:35Z", 
    "id": "oai:repo.scoap3.org:79061", 
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    {
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    {
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        {
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    {
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        {
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        {
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          "value": "Laboratoire de Physique des 2 Infinis, Ir\u00e8ne Joliot-Curie, Orsay, France", 
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    {
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        {
          "country": "USA", 
          "value": "University of Houston, Houston, Texas, United States", 
          "organization": "University of Houston"
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    {
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        {
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          "value": "Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universit\u00e4t Frankfurt, Frankfurt, Germany", 
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    {
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    {
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        {
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          "value": "COMSATS University Islamabad, Islamabad, Pakistan", 
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    {
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        {
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          "value": "University of Tsukuba, Tsukuba, Japan", 
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    {
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          "value": "European Organization for Nuclear Research (CERN), Geneva, Switzerland", 
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        {
          "country": "Czech Republic", 
          "value": "Nuclear Physics Institute of the Czech Academy of Sciences, Husinec-\u0158e\u017e, Czech Republic", 
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      "given_names": "A.", 
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    {
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        {
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          "value": "University of Kansas, Lawrence, Kansas, United States", 
          "organization": "University of Kansas"
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    {
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        {
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          "value": "Saha Institute of Nuclear Physics, Homi Bhabha National Institute, Kolkata, India", 
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    {
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        {
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          "value": "Comenius University Bratislava, Faculty of Mathematics, Physics and Informatics, Bratislava, Slovak Republic", 
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    {
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        {
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          "value": "Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum f\u00fcr Schwerionenforschung GmbH, Darmstadt, Germany", 
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    {
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        {
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          "value": "AGH University of Science and Technology, Cracow, Poland", 
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    {
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        {
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          "value": "Lawrence Berkeley National Laboratory, Berkeley, California, United States", 
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          "value": "European Organization for Nuclear Research (CERN), Geneva, Switzerland", 
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        {
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    {
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        {
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          "value": "Technical University of Ko\u0161ice, Ko\u0161ice, Slovak Republic", 
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    {
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        {
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          "value": "Technical University of Ko\u0161ice, Ko\u0161ice, Slovak Republic", 
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    {
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        {
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          "value": "National Research and Innovation Agency \u2014 BRIN, Jakarta, Indonesia", 
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        {
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          "value": "Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universit\u00e4t Frankfurt, Frankfurt, Germany", 
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        {
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          "value": "Universidade Estadual de Campinas (UNICAMP), Campinas, Brazil", 
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        {
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          "value": "Warsaw University of Technology, Warsaw, Poland", 
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        {
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    {
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        {
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        {
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        {
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        {
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    {
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        {
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          "value": "Institut f\u00fcr Kernphysik, Johann Wolfgang Goethe-Universit\u00e4t Frankfurt, Frankfurt, Germany", 
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    {
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        {
          "country": "Germany", 
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    {
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        {
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        {
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        {
          "country": "Slovakia", 
          "value": "Institute of Experimental Physics, Slovak Academy of Sciences, Ko\u0161ice, Slovak Republic", 
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        {
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          "value": "Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum f\u00fcr Schwerionenforschung GmbH, Darmstadt, Germany", 
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        {
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    {
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      "full_name": "Karasu Uysal, A."
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        {
          "country": "Croatia", 
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    {
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        {
          "country": "Poland", 
          "value": "Warsaw University of Technology, Warsaw, Poland", 
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      "given_names": "E.", 
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        {
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          "value": "Johann-Wolfgang-Goethe Universit\u00e4t Frankfurt Institut f\u00fcr Informatik, Fachbereich Informatik und Mathematik, Frankfurt, Germany", 
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        {
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        {
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          "value": "Institute for Gravitational and Subatomic Physics (GRASP), Utrecht University/Nikhef, Utrecht, Netherlands", 
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          "value": "European Organization for Nuclear Research (CERN), Geneva, Switzerland", 
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    {
      "affiliations": [
        {
          "country": "Germany", 
          "value": "Helmholtz-Institut f\u00fcr Strahlen- und Kernphysik, Rheinische Friedrich-Wilhelms-Universit\u00e4t Bonn, Bonn, Germany", 
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    {
      "affiliations": [
        {
          "country": "China", 
          "value": "Central China Normal University, Wuhan, China", 
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      "full_name": "Khan, S."
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    {
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      "full_name": "Khatun, A."
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    {
      "affiliations": [
        {
          "country": "Poland", 
          "value": "The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland", 
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      "full_name": "Khuntia, A."
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    {
      "affiliations": [
        {
          "country": "South Africa", 
          "value": "University of Cape Town, Cape Town, South Africa", 
          "organization": "University of Cape Town"
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    {
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        {
          "country": "Norway", 
          "value": "Faculty of Engineering and Science, Western Norway University of Applied Sciences, Bergen, Norway", 
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      "full_name": "Kileng, B."
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    {
      "affiliations": [
        {
          "country": "South Korea", 
          "value": "Department of Physics, Pusan National University, Pusan, Republic of Korea", 
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      "surname": "Kim", 
      "given_names": "B.", 
      "full_name": "Kim, B."
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        {
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      "given_names": "C.", 
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    {
      "affiliations": [
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          "country": "Finland", 
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      "surname": "Kim", 
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      "full_name": "Kim, D."
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        {
          "country": "South Korea", 
          "value": "Jeonbuk National University, Jeonju, Republic of Korea", 
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      "surname": "Kim", 
      "given_names": "E.", 
      "full_name": "Kim, E."
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        {
          "country": "South Korea", 
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      "surname": "Kim", 
      "given_names": "J.", 
      "full_name": "Kim, J."
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    {
      "affiliations": [
        {
          "country": "South Korea", 
          "value": "Gangneung-Wonju National University, Gangneung, Republic of Korea", 
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      "surname": "Kim", 
      "given_names": "J.", 
      "full_name": "Kim, J."
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    {
      "affiliations": [
        {
          "country": "Germany", 
          "value": "Physikalisches Institut, Ruprecht-Karls-Universit\u00e4t Heidelberg, Heidelberg, Germany", 
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      "surname": "Kim", 
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      "full_name": "Kim, J."
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    {
      "affiliations": [
        {
          "country": "South Korea", 
          "value": "Jeonbuk National University, Jeonju, Republic of Korea", 
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      "surname": "Kim", 
      "given_names": "J.", 
      "full_name": "Kim, J."
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    {
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        {
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        {
          "country": "Germany", 
          "value": "Physikalisches Institut, Ruprecht-Karls-Universit\u00e4t Heidelberg, Heidelberg, Germany", 
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      "surname": "Kim", 
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      "full_name": "Kim, M."
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    {
      "affiliations": [
        {
          "country": "South Korea", 
          "value": "Department of Physics, Sejong University, Seoul, Republic of Korea", 
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      "full_name": "Kim, S."
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    {
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          "country": "South Korea", 
          "value": "Yonsei University, Seoul, Republic of Korea", 
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      "surname": "Kim", 
      "given_names": "T.", 
      "full_name": "Kim, T."
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    {
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    {
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    {
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    {
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          "value": "Universit\u00e0 di Brescia, Brescia, Italy", 
          "organization": "Universit\u00e0 di Brescia"
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          "value": "INFN, Sezione di Pavia, Pavia, Italy", 
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  "titles": [
    {
      "source": "Springer", 
      "title": "Production of   <math> <msubsup> <mi>K</mi> <mi>S</mi> <mn>0</mn> </msubsup> </math>  $$ {\\textrm{K}}_{\\textrm{S}}^0 $$  , \u039b (  <math> <mover> <mi>\u039b</mi> <mo>\u00af</mo> </mover> </math>  $$ \\overline{\\Lambda} $$ ), \u039e \u00b1 , and \u03a9 \u00b1  in jets and in the underlying event in pp and p\u2013Pb collisions"
    }
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      "value": "10.1007/JHEP07(2023)136"
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      "journal_title": "Journal of High Energy Physics", 
      "material": "article", 
      "journal_volume": "2023", 
      "artid": "JHEP07(2023)136", 
      "year": 2023, 
      "page_start": "1", 
      "journal_issue": "7"
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    "date": "2023-10-24T00:32:45.095395", 
    "source": "Springer", 
    "method": "Springer", 
    "submission_number": "7734084a720411eea066664922b6a1d4"
  }, 
  "page_nr": [
    40
  ], 
  "license": [
    {
      "url": "https://creativecommons.org/licenses//by/4.0", 
      "license": "CC-BY-4.0"
    }
  ], 
  "copyright": [
    {
      "holder": "The Author(s)", 
      "year": "2023"
    }
  ], 
  "control_number": "79061", 
  "collaborations": [
    {
      "value": "The ALICE collaboration"
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      "categories": [
        "nucl-ex", 
        "hep-ex"
      ], 
      "value": "2211.08936"
    }
  ], 
  "abstracts": [
    {
      "source": "Springer", 
      "value": "The production of strange hadrons (  <math> <msubsup> <mi>K</mi> <mi>S</mi> <mn>0</mn> </msubsup> </math>  $$ {\\textrm{K}}_{\\textrm{S}}^0 $$ , \u039b, \u039e \u00b1 , and \u03a9 \u00b1 ), baryon-to-meson ratios (\u039b/   <math> <msubsup> <mi>K</mi> <mi>S</mi> <mn>0</mn> </msubsup> </math>  $$ {\\textrm{K}}_{\\textrm{S}}^0 $$ , \u039e/   <math> <msubsup> <mi>K</mi> <mi>S</mi> <mn>0</mn> </msubsup> </math>  $$ {\\textrm{K}}_{\\textrm{S}}^0 $$ , and \u03a9/   <math> <msubsup> <mi>K</mi> <mi>S</mi> <mn>0</mn> </msubsup> </math>  $$ {\\textrm{K}}_{\\textrm{S}}^0 $$ ), and baryon-to-baryon ratios (\u039e/\u039b, \u03a9/\u039b, and \u03a9/\u039e) associated with jets and the underlying event were measured as a function of transverse momentum (p T) in pp collisions at   <math> <msqrt> <mi>s</mi> </msqrt> </math>  $$ \\sqrt{s} $$  = 13 TeV and p Pb collisions at   <math> <msqrt> <msub> <mi>s</mi> <mi>NN</mi> </msub> </msqrt> </math>  $$ \\sqrt{s_{\\textrm{NN}}} $$  = 5.02 TeV with the ALICE detector at the LHC. The inclusive production of the same particle species and the corresponding ratios are also reported. The production of multi-strange hadrons, \u039e \u00b1  and \u03a9 \u00b1 , and their associated particle ratios in jets and in the underlying event are measured for the first time. In both pp and p\u2013Pb collisions, the baryon-to-meson and baryon-to-baryon yield ratios measured in jets differ from the inclusive particle production for low and intermediate hadron p T (0.6\u20136 GeV/c). Ratios measured in the underlying event are in turn similar to those measured for inclusive particle production. In pp collisions, the particle production in jets is compared with Pythia 8 predictions with three colour-reconnection implementation modes. None of them fully reproduces the data in the measured hadron p T region. The maximum deviation is observed for \u039e \u00b1  and \u03a9 \u00b1  which reaches a factor of about six. The event multiplicity dependence is further investigated in p\u2212Pb collisions. In contrast to what is observed in the underlying event, there is no significant event-multiplicity dependence for particle production in jets. The presented measurements provide novel constraints on hadronisation and its Monte Carlo description. In particular, they demonstrate that the fragmentation of jets alone is insufficient to describe the strange and multi-strange particle production in hadronic collisions at LHC energies."
    }
  ], 
  "imprints": [
    {
      "date": "2023-07-17", 
      "publisher": "Springer"
    }
  ]
}
Published on:
17 July 2023
Publisher:
Springer
Published in:
Journal of High Energy Physics , Volume 2023 (2023)
Issue 7
Pages 1-40
DOI:
https://doi.org/10.1007/JHEP07(2023)136
arXiv:
2211.08936
Copyrights:
The Author(s)
Licence:
CC-BY-4.0

Fulltext files: