Sub-leading flow modes in PbPb collisions at sNN = 2.76 TeV from the HYDJET++ model

  • Recent LHC results on the appearance of sub-leading flow modes in PbPb collisions at 2.76 TeV, related to initial-state fluctuations, are analyzed and interpreted within the HYDJET++ model. Using the newly introduced Principal Component Analysis (PCA) method applied to two-particle azimuthal correlations extracted from the model calculations, the leading and sub-leading flow modes are studied as a function of the transverse momentum (pT) over a wide centrality range. The leading modes of the elliptic (v2(1)) and triangular (v3(1)) flow calculated with the HYDJET++ model reproduce rather well the v2{2} and v3{2} coefficients measured experimentally using the two-particle correlations. Within the pT ≤ 3 GeV/c range, where hydrodynamics dominates, the sub-leading flow effects are greatest at the highest pT of around 3 GeV/c. The sub-leading elliptic flow mode (v2(2)), which corresponds to the n = 2 harmonic, has a small non-zero value and slowly increases from central to peripheral collisions, while the sub-leading triangular flow mode (v3(2)), which corresponds to the n = 3 harmonic, is even smaller and does not depend on centrality. For n = 2, the relative magnitude of the effect measured with respect to the leading flow mode shows a shallow minimum for semi-central collisions and increases for very central and for peripheral collisions. For the n = 3 case, there is no centrality dependence. The sub-leading flow mode results obtained from the HYDJET++ model are in rather good agreement with the experimental measurements of the CMS Collaboration.
      PCAS:
  • 加载中
  • [1] J.-Y. Ollitrault, Phys. Rev. D, 48: 1132-1139 (1993)
    [2] S. Voloshin and Y. Zhang, Z. Phys. C, 70: 665-672 (1996)
    [3] A. M. Poskanzer and S. A. Voloshin, Phys. Rev. C, 58: 1671-1678 (1998)
    [4] B. Alver and G. Roland, Phys. Rev. C, 81: 054905-054913 (2010)
    [5] B.B. Back et al (PHOBOS Collaboration), Phys. Rev. Lett., 89: 222301 (2002)
    [6] K.H. Adams et al (STAR Collaboration), Phys. Rev. Lett., 86: 402-407 (2001)
    [7] K. Adcox et al (PHENIX Collaboration), Phys. Rev. Lett., 89: 212301 (2002)
    [8] K. Aamodt et al (ALICE Collaboration), Phys. Rev. Lett., 105: 252302 (2010)
    [9] K. Aamodt et al (ALICE Collaboration), Phys. Rev. Lett., 107: 032301 (2011)
    [10] B.B. Abelev et al (ALICE Collaboration), JHEP, 1506: 190-271 (2015)
    [11] J. Adam et al (ALICE Collaboration), Phys. Rev. Lett., 116: 132302 (2016)
    [12] G. Aad et al (ATLAS Collaboration), Phys. Lett. B, 707: 330-348 (2012)
    [13] G. Aad et al (ATLAS Collaboration), Phys. Rev. C, 86: 014907-014954 (2012)
    [14] G. Aad et al (ATLAS Collaboration), JHEP, 11: 183-240 (2013)
    [15] S. Chatrchyan et al (CMS Collaboration), Eur. Phys. J. C, 72: 2012 (2012)
    [16] S. Chatrchyan et al (CMS Collaboration), Phys. Rev. C, 87: 014902-014936 (2013)
    [17] S. Chatrchyan et al (CMS Collaboration), Phys. Rev. C, 89: 044906-044937 (2014)
    [18] S. Chatrchyan et al (CMS Collaboration), JHEP, 02: 088-0126 (2014)
    [19] V. Khachatryan et al (CMS Collaboration), Phys. Rev. C, 92: 034911-034937 (2015)
    [20] S. Wang et al, Phys. Rev. C, 44: 1091-1095 (1991)
    [21] F. G. Gardim, F. Grassi, M. Luzum, and J.-Y. Ollitrault, Phys. Rev. C, 87: 031901-031906 (2013)
    [22] U. Heinz, Z. Qiu, and C. Shen, Phys. Rev. C, 87: 034913-034922 (2013)
    [23] Y. Zhou, Nucl. Phys. A, 931: 949-953 (2014)
    [24] R. Bhalerao, J.-I. Ollitrault, S. Pal, and D. Teaney, Phys. Rev. Lett., 114: 152301-152306 (2015)
    [25] A. Mazeliauskas and D. Teaney, Phys. Rev. C, 91: 044902-044912 (2015)
    [26] I. P. Lokhtin, L.V. Malinina, S. V. Petrushanko, A. M. Snigirev, I. Arsene, and K. Tywoniuk, Comput. Phys. Commun., 180: 779-799 (2009)
    [27] T. Sjostrand, S. Mrenna, and P. Skands, JHEP, 0605: 026-0602 (2006)
    [28] I. P. Lokhtin and A. M. Snigirev, Eur. Phys. J. C, 45: 211-217 (2006)
    [29] A. Mazeliauskas and D. Teaney, Phys. Rev. C, 93: 024913-024928 (2016)
    [30] J. Milosevic et al (CMS Collaboration), Nucl. Phys. A, 956: 308-311 (2016)
    [31] S. Chatrchyan et al (CMS Collaboration), Phys. Lett. B, 724: 213-240 (2013)
    [32] K. Aamodt et al (ALICE Collaboration), Phys. Lett. B, 708: 249-264 (2012)
    [33] L. V. Bravina, E. S. Fotina, V. L. Korotkikh, I. P. Lokhtin, L. V. Malinina,E. N. Nazarova, S. V. Petrushanko, A. M. Snigirev, and E. E. Zabrodin, Eur. Phys. J. C, 75, 588-598 (2015)
  • 加载中

Get Citation
P. Cirkovic, D. Devetak, M. Dordevic, J. Milosevic and M. Stojanovic. Sub-leading flow modes in PbPb collisions at sNN = 2.76 TeV from the HYDJET++ model[J]. Chinese Physics C, 2017, 41(7): 074001. doi: 10.1088/1674-1137/41/7/074001
P. Cirkovic, D. Devetak, M. Dordevic, J. Milosevic and M. Stojanovic. Sub-leading flow modes in PbPb collisions at sNN = 2.76 TeV from the HYDJET++ model[J]. Chinese Physics C, 2017, 41(7): 074001.  doi: 10.1088/1674-1137/41/7/074001 shu
Milestone
Received: 2017-02-13
Revised: 2017-03-22
Fund

    Supported by Ministry of Education, Science and Technological Development of the Republic of Serbia (171019)

Article Metric

Article Views(1544)
PDF Downloads(54)
Cited by(0)
Policy on re-use
To reuse of subscription content published by CPC, the users need to request permission from CPC, unless the content was published under an Open Access license which automatically permits that type of reuse.
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Email This Article

Title:
Email:

Sub-leading flow modes in PbPb collisions at sNN = 2.76 TeV from the HYDJET++ model

    Corresponding author: J. Milosevic, Jovan.Milosevic@cern.ch
  • 1.  University of Belgrade and Institute of physics, P.O. Box 68, 11081 Belgrade, Serbia
  • 2.  University of Belgrade and Vinca Institute of Nuclear Sciences, P.O. Box 522, 11001 Belgrade, Serbia
  • 3. University of Belgrade and Vinca Institute of Nuclear Sciences, P.O. Box 522, 11001 Belgrade, Serbia
  • 4. University of Oslo, Department of Physics, Oslo, Norway
Fund Project:  Supported by Ministry of Education, Science and Technological Development of the Republic of Serbia (171019)

Abstract: Recent LHC results on the appearance of sub-leading flow modes in PbPb collisions at 2.76 TeV, related to initial-state fluctuations, are analyzed and interpreted within the HYDJET++ model. Using the newly introduced Principal Component Analysis (PCA) method applied to two-particle azimuthal correlations extracted from the model calculations, the leading and sub-leading flow modes are studied as a function of the transverse momentum (pT) over a wide centrality range. The leading modes of the elliptic (v2(1)) and triangular (v3(1)) flow calculated with the HYDJET++ model reproduce rather well the v2{2} and v3{2} coefficients measured experimentally using the two-particle correlations. Within the pT ≤ 3 GeV/c range, where hydrodynamics dominates, the sub-leading flow effects are greatest at the highest pT of around 3 GeV/c. The sub-leading elliptic flow mode (v2(2)), which corresponds to the n = 2 harmonic, has a small non-zero value and slowly increases from central to peripheral collisions, while the sub-leading triangular flow mode (v3(2)), which corresponds to the n = 3 harmonic, is even smaller and does not depend on centrality. For n = 2, the relative magnitude of the effect measured with respect to the leading flow mode shows a shallow minimum for semi-central collisions and increases for very central and for peripheral collisions. For the n = 3 case, there is no centrality dependence. The sub-leading flow mode results obtained from the HYDJET++ model are in rather good agreement with the experimental measurements of the CMS Collaboration.

    HTML

Reference (33)

目录

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return