{
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  "authors": [
    {
      "raw_name": "M. Petrovici", 
      "affiliations": [
        {
          "country": "Romania", 
          "value": "National Institute for Physics and Nuclear Engineering - IFIN-HH, Hadron Physics Department, Bucharest, Romania"
        }, 
        {
          "country": "Romania", 
          "value": "Faculty of Physics, University of Bucharest, Romania"
        }
      ], 
      "surname": "Petrovici", 
      "given_names": "M.", 
      "full_name": "Petrovici, M."
    }, 
    {
      "raw_name": "A. Lindner", 
      "affiliations": [
        {
          "country": "Romania", 
          "value": "National Institute for Physics and Nuclear Engineering - IFIN-HH, Hadron Physics Department, Bucharest, Romania"
        }, 
        {
          "country": "Romania", 
          "value": "Faculty of Physics, University of Bucharest, Romania"
        }
      ], 
      "surname": "Lindner", 
      "given_names": "A.", 
      "full_name": "Lindner, A."
    }, 
    {
      "raw_name": "A. Pop", 
      "affiliations": [
        {
          "country": "Romania", 
          "value": "National Institute for Physics and Nuclear Engineering - IFIN-HH, Hadron Physics Department, Bucharest, Romania"
        }
      ], 
      "surname": "Pop", 
      "given_names": "A.", 
      "full_name": "Pop, A."
    }, 
    {
      "raw_name": "M. T\u00e2rzil\u0103", 
      "affiliations": [
        {
          "country": "Romania", 
          "value": "National Institute for Physics and Nuclear Engineering - IFIN-HH, Hadron Physics Department, Bucharest, Romania"
        }, 
        {
          "country": "Romania", 
          "value": "Faculty of Physics, University of Bucharest, Romania"
        }
      ], 
      "surname": "T\u00e2rzil\u0103", 
      "given_names": "M.", 
      "full_name": "T\u00e2rzil\u0103, M."
    }, 
    {
      "raw_name": "I. Berceanu", 
      "affiliations": [
        {
          "country": "Romania", 
          "value": "National Institute for Physics and Nuclear Engineering - IFIN-HH, Hadron Physics Department, Bucharest, Romania"
        }
      ], 
      "surname": "Berceanu", 
      "given_names": "I.", 
      "full_name": "Berceanu, I."
    }
  ], 
  "titles": [
    {
      "source": "APS", 
      "title": "Geometrical scaling for energies available at the BNL Relativistic Heavy Ion Collider to those at the CERN Large Hadron Collider"
    }
  ], 
  "dois": [
    {
      "value": "10.1103/PhysRevC.98.024904"
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  "publication_info": [
    {
      "journal_volume": "98", 
      "journal_title": "Physical Review C", 
      "material": "article", 
      "journal_issue": "2", 
      "year": 2018
    }
  ], 
  "$schema": "http://repo.scoap3.org/schemas/hep.json", 
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    "source": "APS", 
    "method": "APS", 
    "submission_number": "bca49440b8c511eaad8602163e01809a"
  }, 
  "page_nr": [
    14
  ], 
  "license": [
    {
      "url": "https://creativecommons.org/licenses/by/4.0/", 
      "license": "CC-BY-4.0"
    }
  ], 
  "copyright": [
    {
      "statement": "Published by the American Physical Society", 
      "year": "2018"
    }
  ], 
  "control_number": "41874", 
  "record_creation_date": "2018-08-07T20:30:19.368318", 
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    {
      "primary": "HEP"
    }, 
    {
      "primary": "Citeable"
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    {
      "primary": "Published"
    }
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  "arxiv_eprints": [
    {
      "categories": [
        "hep-ph", 
        "nucl-th", 
        "25.75Ag, 25.75.Ld, 25.75Nq, 21.65.Qr"
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      "value": "1805.04060"
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  ], 
  "abstracts": [
    {
      "source": "APS", 
      "value": "Based on recent experimental results at the BNL Relativistic Heavy Ion Collider (RHIC) and the CERN Large Hadron Collider (LHC), the <math><mrow><mo>\u2329</mo><msub><mi>p</mi><mi>T</mi></msub><mo>\u232a</mo></mrow></math> dependence of identified light flavor charged hadrons on <math><msqrt><mrow><mrow><mrow><mo>(</mo><mfrac><mrow><mi>d</mi><mi>N</mi></mrow><mrow><mi>d</mi><mi>y</mi></mrow></mfrac><mo>)</mo></mrow><mo>/</mo><msub><mi>S</mi><mo>\u22a5</mo></msub></mrow><mphantom><mpadded width=\"0pt\"><msup><mrow></mrow><mn>2</mn></msup></mpadded></mphantom></mrow></msqrt></math>, the relevant scale in the gluon saturation picture, is studied from <math><mrow><msqrt><msub><mi>s</mi><mi>NN</mi></msub></msqrt><mo>=</mo><mn>7.7</mn></mrow></math> GeV up to 5.02 TeV. This study is extended to the slopes of the <math><mrow><mo>\u2329</mo><msub><mi>p</mi><mi>T</mi></msub><mo>\u232a</mo></mrow></math> dependence on the particle mass and the <math><mrow><mo>\u2329</mo><msub><mi>\u03b2</mi><mi>T</mi></msub><mo>\u232a</mo></mrow></math> parameter from Boltzmann-Gibbs blast wave (BGBW) fits of the <math><msub><mi>p</mi><mi>T</mi></msub></math> spectra. A systematic decrease of the slope of the <math><mrow><mo>\u2329</mo><msub><mi>p</mi><mi>T</mi></msub><mo>\u232a</mo></mrow></math> dependence on <math><msqrt><mrow><mrow><mrow><mo>(</mo><mfrac><mrow><mi>d</mi><mi>N</mi></mrow><mrow><mi>d</mi><mi>y</mi></mrow></mfrac><mo>)</mo></mrow><mo>/</mo><msub><mi>S</mi><mo>\u22a5</mo></msub></mrow><mphantom><mpadded width=\"0pt\"><msup><mrow></mrow><mn>2</mn></msup></mpadded></mphantom></mrow></msqrt></math> from Beam Energy Scan (BES) to LHC energies is evidenced. While, for the RHIC energies, within the experimental errors, <math><mrow><mrow><mo>\u2329</mo><msub><mi>p</mi><mi>T</mi></msub><mo>\u232a</mo></mrow><mo>/</mo><msqrt><mrow><mrow><mrow><mo>(</mo><mfrac><mrow><mi>d</mi><mi>N</mi></mrow><mrow><mi>d</mi><mi>y</mi></mrow></mfrac><mo>)</mo></mrow><mo>/</mo><msub><mi>S</mi><mo>\u22a5</mo></msub></mrow><mphantom><mpadded width=\"0pt\"><msup><mrow></mrow><mn>2</mn></msup></mpadded></mphantom></mrow></msqrt></mrow></math> does not depend on centrality, at the LHC energies a deviation from a linear behavior is observed towards the most central collisions. The influence of the corona contribution on the observed trends is discussed. The slopes of the <math><mrow><mo>\u2329</mo><msub><mi>p</mi><mi>T</mi></msub><mo>\u232a</mo></mrow></math> particle mass dependence and the <math><mrow><mo>\u2329</mo><msub><mi>\u03b2</mi><mi>T</mi></msub><mo>\u232a</mo></mrow></math> parameter from BGBW fits scale well with <math><msqrt><mrow><mrow><mrow><mo>(</mo><mfrac><mrow><mi>d</mi><mi>N</mi></mrow><mrow><mi>d</mi><mi>y</mi></mrow></mfrac><mo>)</mo></mrow><mo>/</mo><msub><mi>S</mi><mo>\u22a5</mo></msub></mrow><mphantom><mpadded width=\"0pt\"><msup><mrow></mrow><mn>2</mn></msup></mpadded></mphantom></mrow></msqrt></math>. Similar systematic trends for <math><mrow><mi>p</mi><mi>p</mi></mrow></math> at <math><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>7</mn></mrow></math> TeV are in a good agreement with the ones corresponding to Pb-Pb collisions at <math><mrow><msqrt><msub><mi>s</mi><mi>NN</mi></msub></msqrt><mo>=</mo><mn>2.76</mn></mrow></math> and 5.02 TeV, pointing to a system-size-independent behavior."
    }
  ], 
  "imprints": [
    {
      "date": "2018-08-07", 
      "publisher": "APS"
    }
  ]
}