{
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  "authors": [
    {
      "raw_name": "P. Castorina", 
      "affiliations": [
        {
          "country": "Italy", 
          "value": "INFN, Sezione di Catania, I-95123 Catania, Italy"
        }, 
        {
          "country": "Czech Republic", 
          "value": "Institute of Particle and Nuclear Physics, Faculty of Mathematics and Physics, Charles University, V Hole\u0161ovi\u010dk\u00e1ch 2, 18000 Prague 8, Czech Republic"
        }
      ], 
      "surname": "Castorina", 
      "given_names": "P.", 
      "full_name": "Castorina, P."
    }, 
    {
      "raw_name": "A. Iorio", 
      "affiliations": [
        {
          "country": "Czech Republic", 
          "value": "Institute of Particle and Nuclear Physics, Faculty of Mathematics and Physics, Charles University, V Hole\u0161ovi\u010dk\u00e1ch 2, 18000 Prague 8, Czech Republic"
        }
      ], 
      "surname": "Iorio", 
      "given_names": "A.", 
      "full_name": "Iorio, A."
    }, 
    {
      "raw_name": "D. Lanteri", 
      "affiliations": [
        {
          "country": "Italy", 
          "value": "INFN, Sezione di Catania, I-95123 Catania, Italy"
        }, 
        {
          "country": "Italy", 
          "value": "Dipartimento di Fisica e Astronomia, Universit\u00e0 di Catania, I-95123 Catania, Italy"
        }
      ], 
      "surname": "Lanteri", 
      "given_names": "D.", 
      "full_name": "Lanteri, D."
    }, 
    {
      "raw_name": "H. Satz", 
      "affiliations": [
        {
          "country": "Germany", 
          "value": "Fakult\u00e4t f\u00fcr Physik, Universit\u00e4t Bielefeld, D-33501 Bielefeld, Germany"
        }
      ], 
      "surname": "Satz", 
      "given_names": "H.", 
      "full_name": "Satz, H."
    }, 
    {
      "raw_name": "M. Spousta", 
      "affiliations": [
        {
          "country": "Czech Republic", 
          "value": "Institute of Particle and Nuclear Physics, Faculty of Mathematics and Physics, Charles University, V Hole\u0161ovi\u010dk\u00e1ch 2, 18000 Prague 8, Czech Republic"
        }
      ], 
      "surname": "Spousta", 
      "given_names": "M.", 
      "full_name": "Spousta, M."
    }
  ], 
  "titles": [
    {
      "source": "APS", 
      "title": "Universality in hadronic and nuclear collisions at high energy"
    }
  ], 
  "dois": [
    {
      "value": "10.1103/PhysRevC.101.054902"
    }
  ], 
  "publication_info": [
    {
      "journal_volume": "101", 
      "journal_title": "Physical Review C", 
      "material": "article", 
      "journal_issue": "5", 
      "year": 2020
    }
  ], 
  "$schema": "http://repo.scoap3.org/schemas/hep.json", 
  "acquisition_source": {
    "date": "2021-08-25T10:41:07.562720", 
    "source": "APS", 
    "method": "APS", 
    "submission_number": "810b323c058f11ecb53772fd3742099d"
  }, 
  "page_nr": [
    5
  ], 
  "license": [
    {
      "url": "https://creativecommons.org/licenses/by/4.0/", 
      "license": "CC-BY-4.0"
    }
  ], 
  "copyright": [
    {
      "statement": "Published by the American Physical Society", 
      "year": "2020"
    }
  ], 
  "control_number": "54313", 
  "record_creation_date": "2020-05-11T18:30:07.152327", 
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  "collections": [
    {
      "primary": "HEP"
    }, 
    {
      "primary": "Citeable"
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    {
      "primary": "Published"
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  ], 
  "arxiv_eprints": [
    {
      "categories": [
        "hep-ph", 
        "nucl-th"
      ], 
      "value": "1912.12513"
    }
  ], 
  "abstracts": [
    {
      "source": "APS", 
      "value": "Recent experimental results in proton-proton and in proton-nucleus collisions at Large Hadron Collider energies show a strong similarity to those observed in nucleus-nucleus collisions, where the formation of a quark-gluon plasma is expected. We discuss the comparison between small colliding systems and nucleus-nucleus collisions, for (a) the strangeness suppression factor <math><msub><mi>\u03b3</mi><mi>s</mi></msub></math> and yields of multi-strange hadrons; (b) the average transverse momentum, <math><msub><mi>p</mi><mi>t</mi></msub></math>, with particular attention to the low <math><msub><mi>p</mi><mi>t</mi></msub></math> region where soft, nonperturbative effects are important; and (c) the elliptic flow scaled by the participant eccentricity. The universal behavior in hadronic and nuclear high energy collisions emerges for all these observables in terms of a specific dynamical variable which corresponds to the entropy density of initial system in the collision and which takes into account the transverse size of the initial configuration and its fluctuations."
    }
  ], 
  "imprints": [
    {
      "date": "2020-05-11", 
      "publisher": "APS"
    }
  ]
}