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Exploring new small system geometries in heavy ion collisions

S. H. Lim, J. Carlson, C. Loizides, D. Lonardoni, J. E. Lynn, J. L. Nagle, J. D. Orjuela Koop, and J. Ouellette
Phys. Rev. C 99, 044904 – Published 4 April 2019

Abstract

Relativistic heavy ion collisions produce nuclei-sized droplets of quark-gluon plasma whose expansion is well described by viscous hydrodynamic calculations. Over the past half decade, this formalism was also found to apply to smaller droplets closer to the size of individual nucleons, as produced in p+p and p+A collisions. The hydrodynamic paradigm was further tested with a variety of collision species, including p+Au,d+Au, and He3+Au producing droplets with different geometries. Nevertheless, questions remain regarding the importance of pre-hydrodynamic evolution and the exact medium properties during the hydrodynamic evolution phase, as well as the applicability of alternative theories that argue the agreement with hydrodynamics is accidental. In this work we explore options for new collision geometries including p+O and O+O proposed for running at the Large Hadron Collider, as well as He4+Au,C+Au,O+Au, and Be7,9+Au at the Relativistic Heavy Ion Collider.

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  • Received 31 December 2018

DOI:https://doi.org/10.1103/PhysRevC.99.044904

©2019 American Physical Society

Physics Subject Headings (PhySH)

Nuclear Physics

Authors & Affiliations

S. H. Lim1, J. Carlson2, C. Loizides3, D. Lonardoni4,2, J. E. Lynn5,6, J. L. Nagle1,7, J. D. Orjuela Koop1, and J. Ouellette1

  • 1University of Colorado, Boulder, Colorado 80309, USA
  • 2Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
  • 3Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 4Facility for Rare Isotope Beams, Michigan State University, East Lansing, Michigan 48824, USA
  • 5Institut für Kernphysik, Technische Universität Darmstadt, D-64289 Darmstadt, Germany
  • 6ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, D-64291 Darmstadt, Germany
  • 7CEA/IPhT/Saclay, F-Orsay, 91190, France

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Issue

Vol. 99, Iss. 4 — April 2019

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Images

  • Figure 1
    Figure 1

    Mean eccentricity (ɛ2,ɛ3,ɛ4) as a function of impact parameter in p+O and O+O collisions at sNN=7TeV.

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  • Figure 2
    Figure 2

    dNch/dη at midrapidity from sonic in unbiased (0%–100%) p+O and O+O collisions at sNN=7TeV, and the shaded region is corresponding to 5% events of highest dNch/dη.

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  • Figure 3
    Figure 3

    An example of time evolution of a O+O event from sonic; the color scale indicates the local temperature.

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  • Figure 4
    Figure 4

    Comparison of vn and vn/ɛn as a function of pT in 0%–5% of three collision systems, p+O and O+O collisions at sNN=7TeV and p+Pb collisions at sNN=8.16TeV.

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  • Figure 5
    Figure 5

    Comparison of vn and vn/ɛn as a function of pT in a 5% centrality range of collisions showing a similar dNch/dη.

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  • Figure 6
    Figure 6

    Comparison of the mean eccentricity as a function of impact parameter in O+O collisions between MC Glauber and IP-Jazma initial conditions.

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  • Figure 7
    Figure 7

    Comparison of dNch/dη,vn, and vn/ɛn in O+O collisions at sNN=7 TeV from sonic between MC Glauber and IP-Jazma initial conditions.

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  • Figure 8
    Figure 8

    Mean eccentricity (ɛ2,ɛ3,ɛ4) as a function of impact parameter in He3+Au and He4+Au collisions at sNN=200GeV.

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  • Figure 9
    Figure 9

    An example of time evolution of a He4+Au event from sonic; the color scale indicates the local temperature.

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  • Figure 10
    Figure 10

    Comparison of vn and vn/ɛn from sonic as a function of pT in 0%–5% of He3+Au and He4+Au collisions at sNN=200GeV.

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  • Figure 11
    Figure 11

    Comparison of vn and vn/ɛn from sonic as a function of pT in 0%–5% of He3+Au and 5%–10% of He4+Au collisions at sNN=200GeV.

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  • Figure 12
    Figure 12

    Spatial triangularity ɛ3 is shown as a function of number of nucleon participants for C+Au (left) and O+Au (right) collisions at sNN=200 GeV. Results are shown utilizing the full 12- and 16-nucleon configurations (black), the reshuffled nucleon configurations with no correlations (red), and with the toy geometry model involving simple triangles and tetrahedra (blue).

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  • Figure 13
    Figure 13

    Number of participating nucleons in minimum bias p+O (left) and O+O (right) collisions from Monte Calro Glauber calculations. Shown are the results of two oxygen cases, one with the full 16-nucleon configurations and one with the simple α-cluster tetrahedron configuration.

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  • Figure 14
    Figure 14

    An example of time evolution of a Be9+Au event from sonic, and the color scale indicates the local temperature. In this event, one can see the distinct hot spots from the two α clusters and the extra neutron from the Be9 projectile.

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  • Figure 15
    Figure 15

    Mean charged particle production per pair participant (dNch/dη/(Npart/2)) for p+Pb, Pb+Pb, and O+O collisions in ampt at sNN=5.02 TeV with the same Lund string fragmentation function parameters (a=0.3,b=0.15). Measurements by the ALICE collaboration in Pb+Pb collisions [47] are shown for comparison.

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  • Figure 16
    Figure 16

    Flow coefficients vn as a function of pT in the highest 0%–5% centrality class in p+O (a)–(c) and O+O (d)–(f) collisions at sNN=7 TeV, as calculated with the ampt model. Two calculations are presented, namely the true flow vn{PP} relative to the parton participant plane, and the two-particle correlation flow vn{2PC}.

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