{
  "_oai": {
    "updated": "2022-03-03T22:29:02Z", 
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  "authors": [
    {
      "raw_name": "Kevin Dusling", 
      "affiliations": [
        {
          "country": "USA", 
          "value": "American Physical Society, 1 Research Road, Ridge, New York 11961, USA"
        }, 
        {
          "country": "USA", 
          "value": "Physics Department, Brookhaven National Laboratory, Bldg. 510A, Upton, New York 11973, USA"
        }
      ], 
      "surname": "Dusling", 
      "given_names": "Kevin", 
      "full_name": "Dusling, Kevin"
    }, 
    {
      "raw_name": "Mark Mace", 
      "affiliations": [
        {
          "country": "USA", 
          "value": "Physics Department, Brookhaven National Laboratory, Bldg. 510A, Upton, New York 11973, USA"
        }, 
        {
          "country": "USA", 
          "value": "Physics and Astronomy Department, Stony Brook University, Stony Brook, New York 11974, USA"
        }
      ], 
      "surname": "Mace", 
      "given_names": "Mark", 
      "full_name": "Mace, Mark"
    }, 
    {
      "raw_name": "Raju Venugopalan", 
      "affiliations": [
        {
          "country": "USA", 
          "value": "Physics Department, Brookhaven National Laboratory, Bldg. 510A, Upton, New York 11973, USA"
        }
      ], 
      "surname": "Venugopalan", 
      "given_names": "Raju", 
      "full_name": "Venugopalan, Raju"
    }
  ], 
  "titles": [
    {
      "source": "APS", 
      "title": "Parton model description of multiparticle azimuthal correlations in <math><mi>p</mi><mi>A</mi></math> collisions"
    }
  ], 
  "dois": [
    {
      "value": "10.1103/PhysRevD.97.016014"
    }
  ], 
  "publication_info": [
    {
      "journal_volume": "97", 
      "journal_title": "Physical Review D", 
      "material": "article", 
      "journal_issue": "1", 
      "year": 2018
    }
  ], 
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    "date": "2020-06-29T15:40:53.512518", 
    "source": "APS", 
    "method": "APS", 
    "submission_number": "b8bb8f3cb9e211eaad8602163e01809a"
  }, 
  "page_nr": [
    21
  ], 
  "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": "23329", 
  "record_creation_date": "2018-06-08T06:05:46.978112", 
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  "collections": [
    {
      "primary": "HEP"
    }, 
    {
      "primary": "Citeable"
    }, 
    {
      "primary": "Published"
    }
  ], 
  "arxiv_eprints": [
    {
      "categories": [
        "hep-ph", 
        "nucl-ex", 
        "nucl-th"
      ], 
      "value": "1706.06260"
    }
  ], 
  "abstracts": [
    {
      "source": "APS", 
      "value": "In K. Dusling et al. [arXiv:1705.00745.], an initial-state \u201cparton model\u201d of quarks scattering off a dense nuclear target was shown to qualitatively reproduce the systematics of multiparticle azimuthal anisotropy cumulants measured in proton/deuteron-nucleus (<math><mi>p</mi><mi>A</mi></math>) collisions at the Relativistic Heavy Ion Collider and the LHC. The systematics included (i) the behavior of the four-particle cumulant <math><msub><mi>c</mi><mn>2</mn></msub><mo>{</mo><mn>4</mn><mo>}</mo></math>, which generates a real four-particle second Fourier harmonic <math><msub><mi>v</mi><mn>2</mn></msub><mo>{</mo><mn>4</mn><mo>}</mo></math>; (ii) the ordering <math><msub><mi>v</mi><mn>2</mn></msub><mo>{</mo><mn>2</mn><mo>}</mo><mo>&gt;</mo><msub><mi>v</mi><mn>2</mn></msub><mo>{</mo><mn>4</mn><mo>}</mo><mo>\u2248</mo><msub><mi>v</mi><mn>2</mn></msub><mo>{</mo><mn>6</mn><mo>}</mo><mo>\u2248</mo><msub><mi>v</mi><mn>2</mn></msub><mo>{</mo><mn>8</mn><mo>}</mo></math> for two-, four-, six-, and eight-particle Fourier harmonics; and (iii) the behavior of so-called symmetric cumulants SC(2,3) and SC(2,4). These features of azimuthal multiparticle cumulants were previously interpreted as a signature of hydrodynamic flow; our results challenge this interpretation. We expand here upon our previous study and present further details and novel results on the saturation scale and transverse momentum (<math><msub><mi>p</mi><mo>\u22a5</mo></msub></math>) dependence of multiparticle azimuthal correlations. We find that the dependence of <math><msub><mi>v</mi><mn>2</mn></msub><mo>{</mo><mn>2</mn><mo>}</mo></math> and <math><msub><mi>v</mi><mn>2</mn></msub><mo>{</mo><mn>4</mn><mo>}</mo></math> on the number of color domains in the target varies with the <math><msub><mi>p</mi><mo>\u22a5</mo></msub></math> window explored. We extend our prior discussion of symmetric cumulants and compute as yet unmeasured symmetric cumulants. We investigate the <math><msub><mi>N</mi><mi>c</mi></msub></math> dependence of <math><msub><mi>v</mi><mn>2</mn></msub><mo>{</mo><mn>2</mn><mo>}</mo></math> and <math><msub><mi>v</mi><mn>2</mn></msub><mo>{</mo><mn>4</mn><mo>}</mo></math>. We contrast our results, which include multiple scatterings of each quark off the target, to the Glasma graph approximation, where each quark suffers at most two-gluon exchanges with the target. We find that coherent multiple scattering is essential to obtain a positive definite <math><msub><mi>v</mi><mn>2</mn></msub><mo>{</mo><mn>4</mn><mo>}</mo></math>. We provide an algorithm to compute expectation values of arbitrary products of the \u201cdipole\u201d lightlike Wilson line correlators."
    }
  ], 
  "imprints": [
    {
      "date": "2018-01-25", 
      "publisher": "APS"
    }
  ]
}