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

Shuzhe Shi; Jinfeng Liao; Miklos Gyulassy

doi:10.1088/1674-1137/42/10/104104

Chinese Physics C> 2018, Vol. 42> Issue(10) : 104104 DOI: 10.1088/1674-1137/42/10/104104

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 &

Abstract
HTML
Reference
Related

PDF

Abstract：
We develop a comprehensive dynamical framework, CIBJET, to calculate on an event-by-event basis the dependence of correlations between soft (p_T<2 GeV) and hard (p_T> 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.
- quark-gluon plasma ,
- heavy ion collision ,
- jet quenching ,
- confinement

References

[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]

[1]	Qi Zhou , Ben-Wei Zhang . ${\mathcal{{{R}}}^{\boldsymbol{2}}}$ curvature-squared corrections on Langevin diffusion coefficients. Chinese Physics C, 2025, 49(1): 014105. doi: 10.1088/1674-1137/ad8420
[2]	Shu-Qing Li , Wen-Jing Xing , Shanshan Cao , Guang-You Qin . Quenching and flow of charm and bottom quarks via semi-leptonic decay of D and B mesons in Pb+Pb collisions at the LHC. Chinese Physics C, 2024, 48(8): 084106. doi: 10.1088/1674-1137/ad4c59
[3]	Sa Wang , Wei Dai , Ben-Wei Zhang , Enke Wang . Z⁰ boson associated b-jet production in high-energy nuclear collisions. Chinese Physics C, 2023, 47(5): 054102. doi: 10.1088/1674-1137/acc1ca
[4]	Mengxue Zhang , Yang He , Shanshan Cao , Li Yi . Effects of the formation time of parton shower on jet quenching in heavy-ion collisions. Chinese Physics C, 2023, 47(2): 024106. doi: 10.1088/1674-1137/aca4c1
[5]	Qing Zhang , Wei Dai , Lei Wang , Ben-Wei Zhang , Enke Wang . Particle production at large p_T in Xe+Xe collisions with jet quenching using the higher twist approach. Chinese Physics C, 2022, 46(10): 104106. doi: 10.1088/1674-1137/ac7b75
[6]	Bing-feng Jiang , Shao-wu Shi , De-fu Hou , Jia-rong Li . Color-electric conductivity in a viscous quark-gluon plasma. Chinese Physics C, 2021, 45(5): 054106. doi: 10.1088/1674-1137/abe9a2
[7]	Ismat Ullah , Min He . Modification of the spectra of correlated charm-anticharm quark pairs in the quark-gluon plasma. Chinese Physics C, 2020, 44(5): 054102. doi: 10.1088/1674-1137/44/5/054102
[8]	Shu-Qing Li , Wen-Jing Xing , Feng-Lei Liu , Shanshan Cao , Guang-You Qin . Heavy flavor quenching and flow: the roles of initial condition, pre-equilibrium evolution, and in-medium interaction. Chinese Physics C, 2020, 44(11): 114101. doi: 10.1088/1674-1137/abadee
[9]	Yin Jiang , Shuzhe Shi , Yi Yin , Jinfeng Liao . Quantifying the chiral magnetic effect from anomalous-viscous fluid dynamics. Chinese Physics C, 2018, 42(1): 011001. doi: 10.1088/1674-1137/42/1/011001
[10]	Hao-Jie Xu , Jie Zhao , Xiao-Bao Wang , Han-Lin Li , Zi-Wei Lin , Cai-Wan Shen , Fu-Qiang Wang . Varying the chiral magnetic effect relative to flow in a single nucleus-nucleus collision. Chinese Physics C, 2018, 42(8): 084103. doi: 10.1088/1674-1137/42/8/084103
[11]	Ren-Zhuo Wan , Si-Yuan Wang , Shuang Li , Yi-Ming Feng , Feng Liu , Fan Yang , Dai-Cui Zhou . Large angle radiation effect on jet measurement in pp collisions at s=7 TeV at the LHC. Chinese Physics C, 2018, 42(11): 114001. doi: 10.1088/1674-1137/42/11/114001
[12]	Jong-Ping Hsu . Quark confinement, new cosmic expansion and general Yang-Mills symmetry. Chinese Physics C, 2017, 41(1): 015101. doi: 10.1088/1674-1137/41/1/015101
[13]	. Addendum: Quark Confinement, New Cosmic Expansion and General Yang-Mills Symmetry. Chinese Physics C, 2017, 41(12): 129102.
[14]	SONG Zi-Feng , TANG Qi , LIU Zhong-Jie , ZHAN Xia-Yu , CHEN Jia-Bin . An improved method of unfolding neutron TOF spectrum for low ion temperature inertial confinement fusion. Chinese Physics C, 2014, 38(6): 066201. doi: 10.1088/1674-1137/38/6/066201
[15]	LI De-Sheng , TIAN Feng-Ge , CHEN Gang . Study on the method of mini-jet identification in relativistic heavy ion collisions. Chinese Physics C, 2011, 35(9): 833-837. doi: 10.1088/1674-1137/35/9/009
[16]	WANG Hai-Jun , GENG Wen-Tong . Quark confinement and the fractional quantum Hall effect. Chinese Physics C, 2008, 32(9): 705-709. doi: 10.1088/1674-1137/32/9/006
[17]	Zeng Xianghua , Ge Lingxiao . Thermalization,Expansion, and Radial Flow in HIC. Chinese Physics C, 1997, 21(S2): 47-52.
[18]	Li Panlin , Wu Hua , Xu Mengjie . Dynamics of Phase Transition Including Quark-Fragment Effects for an Expansion Quark-Gluon Plasma. Chinese Physics C, 1997, 21(S4): 55-64.
[19]	Liu Bo , Zhao Weiqin . Analysis of the New Data of Transverse Energy Distributions in High Energy p-A Collisions Based on Geometrical Model. Chinese Physics C, 1994, 18(S4): 385-390.
[20]	Zhang Xiaofei , Li Jiarong . Calculation of Transport Coefficients for Colored Plasma Beyond the Abelian Dominance Approximation. Chinese Physics C, 1994, 18(S4): 375-384.

Access

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

RIS(for EndNote,Reference Manager,ProCite)

BibTex

Txt

Milestone

Received: 2018-07-08

Fund

Supported by National Science Foundation (PHY-1352368).

Article Metric

Article Views(1619)
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

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

Abstract：

References

Access

Article Metrics

Metrics

通讯作者: 陈斌, bchen63@163.com

Email This Article

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

HTML

目录