×
近期发现有不法分子冒充我刊与作者联系,借此进行欺诈等不法行为,请广大作者加以鉴别,如遇诈骗行为,请第一时间与我刊编辑部联系确认(《中国物理C》(英文)编辑部电话:010-88235947,010-88236950),并作报警处理。
本刊再次郑重声明:
(1)本刊官方网址为cpc.ihep.ac.cn和https://iopscience.iop.org/journal/1674-1137
(2)本刊采编系统作者中心是投稿的唯一路径,该系统为ScholarOne远程稿件采编系统,仅在本刊投稿网网址(https://mc03.manuscriptcentral.com/cpc)设有登录入口。本刊不接受其他方式的投稿,如打印稿投稿、E-mail信箱投稿等,若以此种方式接收投稿均为假冒。
(3)所有投稿均需经过严格的同行评议、编辑加工后方可发表,本刊不存在所谓的“编辑部内部征稿”。如果有人以“编辑部内部人员”名义帮助作者发稿,并收取发表费用,均为假冒。
                  
《中国物理C》(英文)编辑部
2024年10月30日

Probing the color structure of the perfect QCD fluids via soft-hard-event-by-event azimuthal correlations

  • We develop a comprehensive dynamical framework, CIBJET, to calculate on an event-by-event basis the dependence of correlations between soft (pT<2 GeV) and hard (pT> 10 GeV) azimuthal flow angle harmonics on the color composition of near-perfect QCD fluids produced in high energy nuclear collisions at RHIC and LHC. CIBJET combines consistently predictions of event-by-event VISHNU2+1 viscous hydrodynamic fluid fields with CUJET3.1 predictions of event-by-event jet quenching. We find that recent correlation data favor a temperature dependent color composition including bleached chromo-electric q(T)+g(T) components and an emergent chromo-magnetic degrees of freedom m(T) consistent with non-perturbative lattice QCD information in the confinement/deconfinement temperature range.
      PCAS:
  • 加载中
  • [1] M. Gyulassy and L. McLerran, Nucl. Phys. A, 750:30 (2005)
    [2] E. V. Shuryak, Nucl. Phys. A, 750:64 (2005)
    [3] P. Jacobs and X. N. Wang, Prog. Part. Nucl. Phys., 54:443 (2005), doi:10.1016/j.ppnp.2004.09.001,[hep-ph/0405125]
    [4] B. Muller, J. Schukraft, and B. Wyslouch, Ann. Rev. Nucl. Part. Sci., 62:361 (2012)
    [5] E. Shuryak, Rev. Mod. Phys., 89:035001 (2017)
    [6] A. Bazavov et al, Equation of state and QCD transition at finite temperature, Phys. Rev. D, 80:014504 (2009), doi:10.1103/PhysRevD.80.014504, arXiv:0903.4379[hep-lat]
    [7] S. Borsanyi et al (Wuppertal-Budapest Collaboration), JHEP, 1009:073 (2010), doi:10.1007/JHEP09(2010)073, arXiv:1005.3508[hep-lat]
    [8] P. Danielewicz and M. Gyulassy, Phys. Rev. D, 31:53 (1985)
    [9] P. Kovtun, D. T. Son, and A. O. Starinets, Phys. Rev. Lett., 94:111601 (2005), doi:10.1103/PhysRevLett.94.111601,[hep-th/0405231]
    [10] J. Xu, A. Buzzatti, and M. Gyulassy, JHEP, 1408:063 (2014), doi:10.1007/JHEP08(2014)063, arXiv:1402.2956[hep-ph]
    [11] J. Xu, J. Liao, and M. Gyulassy, Chin. Phys. Lett., 32(9):092501 (2015), doi:10.1088/0256-307X/32/9/092501, arXiv:1411.3673[hep-ph]
    [12] J. Xu, J. Liao, and M. Gyulassy, JHEP, 1602:169 (2016), doi:10.1007/JHEP02(2016)169, arXiv:1508.00552[hep-ph]
    [13] S. Shi, J. Xu, J. Liao, and M. Gyulassy, Nucl. Phys. A, 967:648 (2017), doi:10.1016/j.nuclphysa.2017.06.037, arXiv:1704.04577[hep-ph]
    [14] S. Shi, J. Liao, and M. Gyulassy, to appear soon
    [15] J. Liao and E. Shuryak, Phys. Rev. Lett., 102:202302 (2009), doi:10.1103/PhysRevLett.102.202302, arXiv:0810.4116[nucl-th]
    [16] B. Betz and M. Gyulassy, Phys. Rev. C, 86:024903 (2012), doi:10.1103/PhysRevC.86.024903, arXiv:1201.0281[nucl-th]
    [17] B. Betz and M. Gyulassy, JHEP, 1408:090 (2014); JHEP, 1410:043 (2014), doi:10.1007/JHEP10(2014)043, 10.1007/JHEP08(2014)090, arXiv:1404.6378[hep-ph]
    [18] X. Zhang and J. Liao, Phys. Rev. C, 89(1):014907 (2014), doi:10.1103/PhysRevC.89.014907, arXiv:1208.6361[nucl-th]
    [19] X. Zhang and J. Liao, Phys. Rev. C, 87:044910 (2013), doi:10.1103/PhysRevC.87.044910, arXiv:1210.1245[nucl-th]
    [20] D. Li, J. Liao, and M. Huang, Phys. Rev. D, 89(12):126006 (2014), doi:10.1103/PhysRevD.89.126006, arXiv:1401.2035[hep-ph]
    [21] S. K. Das, F. Scardina, S. Plumari, and V. Greco, Phys. Lett. B, 747:260 (2015)
    [22] M. Gyulassy, I. Vitev, and X. N. Wang, Phys. Rev. Lett., 86:2537 (2001), doi:10.1103/PhysRevLett.86.2537,[nucl-th/0012092].
    [23] J. Noronha-Hostler, B. Betz, J. Noronha, and M. Gyulassy, Phys. Rev. Lett., 116(25):252301 (2016), doi:10.1103/PhysRevLett.116.252301, arXiv:1602.03788[nucl-th]
    [24] B. Betz, M. Gyulassy, M. Luzum, J. Noronha, J. Noronha-Hostler, I. Portillo, and C. Ratti, Phys. Rev. C, 95(4):044901 (2017), doi:10.1103/PhysRevC.95.044901, arXiv:1609.05171[nucl-th]
    [25] B. G. Zakharov, JETP Lett., 101(9):587 (2015)[Pisma Zh. Eksp. Teor. Fiz., 101(9):659 (2015)], doi:10.1134/S0021364015090131, arXiv:1412.6287[hep-ph]
    [26] C. Shen, Z. Qiu, H. Song, J. Bernhard, S. Bass, and U. Heinz, Comput. Phys. Commun., 199:61 (2016), doi:10.1016/j.cpc.2015.08.039, arXiv:1409.8164[nucl-th]
    [27] J. S. Moreland, J. E. Bernhard, and S. A. Bass, Phys. Rev. C, 92(1):011901 (2015), doi:10.1103/PhysRevC.92.011901, arXiv:1412.4708[nucl-th]
    [28] A. Buzzatti and M. Gyulassy, Phys. Rev. Lett., 108:022301 (2012), doi:10.1103/PhysRevLett.108.022301, arXiv:1106.3061[hep-ph]
    [29] M. H. Thoma and M. Gyulassy, Nucl. Phys. B, 351:491 (1991)
    [30] M. Gyulassy, P. Levai, and I. Vitev, Nucl. Phys. B, 594:371 (2001)
    [31] M. Djordjevic and M. Gyulassy, Nucl. Phys. A, 733:265 (2004)
    [32] S. Wicks, W. Horowitz, M. Djordjevic, and M. Gyulassy, Nucl. Phys. A, 784:426 (2007)
    [33] Y. Hidaka and R. D. Pisarski, Phys. Rev. D, 78:071501 (2008), doi:10.1103/PhysRevD.78.071501, arXiv:0803.0453[hep-ph]
    [34] Y. Hidaka and R. D. Pisarski, Phys. Rev. D, 81:076002 (2010), doi:10.1103/PhysRevD.81.076002, arXiv:0912.0940[hep-ph]
    [35] S. Lin, R. D. Pisarski, and V. V. Skokov, Phys. Lett. B, 730:236 (2014), doi:10.1016/j.physletb.2014.01.043, arXiv:1312.3340[hep-ph]
    [36] J. Liao and E. Shuryak, Phys. Rev. C, 75:054907 (2007), doi:10.1103/PhysRevC.75.054907,[hep-ph/0611131]
    [37] J. Liao and E. Shuryak, Phys. Rev. C, 77:064905 (2008), doi:10.1103/PhysRevC.77.064905, arXiv:0706.4465[hep-ph]
    [38] J. Liao and E. Shuryak, Phys. Rev. Lett., 101:162302 (2008), doi:10.1103/PhysRevLett.101.162302, arXiv:0804.0255[hep-ph]
    [39] C. Ratti and E. Shuryak, Phys. Rev. D, 80:034004 (2009), doi:10.1103/PhysRevD.80.034004, arXiv:0811.4174[hep-ph]
    [40] A. D'Alessandro and M. D'Elia, Nucl. Phys. B, 799:241 (2008), doi:10.1016/j.nuclphysb.2008.03.002, arXiv:0711.1266[hep-lat]
    [41] C. Bonati and M. D'Elia, Nucl. Phys. B, 877:233 (2013), doi:10.1016/j.nuclphysb.2013.10.004, arXiv:1308.0302[hep-lat]
    [42] S. Acharya et al (ALICE Collaboration), arXiv:1802.09145[nucl-ex]
    [43] The ATLAS collaboration (ATLAS Collaboration), ATLAS-CONF-2017-012
    [44] V. Khachatryan et al (CMS Collaboration), JHEP, 1704:039 (2017), doi:10.1007/JHEP04(2017)039, arXiv:1611.01664[nucl-ex]
    [45] A. M. Sirunyan et al (CMS Collaboration), Phys. Lett. B, 776:195 (2018), doi:10.1016/j.physletb.2017.11.041, arXiv:1702.00630[hep-ex]
    [46] J. Adam et al (ALICE Collaboration), Phys. Rev. Lett., 116(13):132302 (2016), doi:10.1103/PhysRevLett.116.132302, arXiv:1602.01119[nucl-ex]
    [47] S. Cao, L. G. Pang, T. Luo, Y. He, G. Y. Qin, and X. N. Wang, Nucl. Part. Phys. Proc., 289-290:217 (2017)
    [48] S. Cao, T. Luo, G. Y. Qin, and X. N. Wang, Phys. Lett. B, 777:255 (2018)
    [49] E. Bianchi, J. Elledge, A. Kumar, A. Majumder, G. Y. Qin, and C. Shen, arXiv:1702.00481[nucl-th]
    [50] Y. T. Chien, A. Emerman, Z. B. Kang, G. Ovanesyan, and I. Vitev, Phys. Rev. D, 93(7):074030 (2016)
    [51] M. Djordjevic, M. Djordjevic, and B. Blagojevic, Phys. Lett. B, 737:298 (2014)
    [52] R. Rapp et al, arXiv:1803.03824[nucl-th]
    [53] S. Chatrchyan et al (CMS Collaboration), Phys. Rev. Lett., 109:022301 (2012), doi:10.1103/PhysRevLett.109.022301, arXiv:1204.1850[nucl-ex]
    [54] A. Ramamurti and E. Shuryak, Phys. Rev. D, 97(1):016010 (2018), doi:10.1103/PhysRevD.97.016010, arXiv:1708.04254[hep-ph]
    [55] K. M. Burke et al (JET Collaboration), Phys. Rev. C, 90(1):014909 (2014), doi:10.1103/PhysRevC.90.014909, arXiv:1312.5003[nucl-th]
    [56] H. Liu, K. Rajagopal, and U. A. Wiedemann, Phys. Rev. Lett., 97:182301 (2006) doi:10.1103/PhysRevLett.97.182301[hep-ph/0605178]
  • 加载中

Get Citation
Shuzhe Shi, Jinfeng Liao and Miklos Gyulassy. Probing the color structure of the perfect QCD fluids via soft-hard-event-by-event azimuthal correlations[J]. Chinese Physics C, 2018, 42(10): 104104. doi: 10.1088/1674-1137/42/10/104104
Shuzhe Shi, Jinfeng Liao and Miklos Gyulassy. Probing the color structure of the perfect QCD fluids via soft-hard-event-by-event azimuthal correlations[J]. Chinese Physics C, 2018, 42(10): 104104.  doi: 10.1088/1674-1137/42/10/104104 shu
Milestone
Received: 2018-07-08
Fund

    Supported by National Science Foundation (PHY-1352368).

Article Metric

Article Views(1584)
PDF Downloads(32)
Cited by(0)
Policy on re-use
To reuse of Open Access content published by CPC, for content published under the terms of the Creative Commons Attribution 3.0 license (“CC CY”), the users don’t need to request permission to copy, distribute and display the final published version of the article and to create derivative works, subject to appropriate attribution.
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:

Probing the color structure of the perfect QCD fluids via soft-hard-event-by-event azimuthal correlations

  • 1.  Physics Department and Center for Exploration of Energy and Matter, Indiana University, 2401 N Milo B. Sampson Lane, Bloomington, IN 47408, USA
  • 2. Nuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA
  • 3. Pupin Lab MS-5202, Department of Physics, Columbia University, New York, NY 10027, USA
  • 4. Institute of Particle Physics and Key Laboratory of Quark &
Fund Project:  Supported by National Science Foundation (PHY-1352368).

Abstract: We develop a comprehensive dynamical framework, CIBJET, to calculate on an event-by-event basis the dependence of correlations between soft (pT<2 GeV) and hard (pT> 10 GeV) azimuthal flow angle harmonics on the color composition of near-perfect QCD fluids produced in high energy nuclear collisions at RHIC and LHC. CIBJET combines consistently predictions of event-by-event VISHNU2+1 viscous hydrodynamic fluid fields with CUJET3.1 predictions of event-by-event jet quenching. We find that recent correlation data favor a temperature dependent color composition including bleached chromo-electric q(T)+g(T) components and an emergent chromo-magnetic degrees of freedom m(T) consistent with non-perturbative lattice QCD information in the confinement/deconfinement temperature range.

    HTML

Reference (56)

目录

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return