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Observation of the Electromagnetic Field Effect via Charge-Dependent Directed Flow in Heavy-Ion Collisions at the Relativistic Heavy Ion Collider

M. I. Abdulhamid4, B. E. Aboona55, J. Adam15, J. R. Adams40, G. Agakishiev30, I. Aggarwal41, M. M. Aggarwal41, Z. Ahammed61, A. Aitbaev30 et al. (STAR Collaboration)

A. Aitbaev30, I. Alekseev2,37, E. Alpatov37, A. Aparin30, S. Aslam26, J. Atchison1, G. S. Averichev30, V. Bairathi53, J. G. Ball Cap22, K. Barish11, P. Bhagat29, A. Bhasin29, S. Bhatta52, S. R. Bhosale17, I. G. Bordyuzhin2, J. D. Brandenburg40, A. V. Brandin37, X. Z. Cai50, H. Caines64, M. Calderón de la Barca Sánchez9, D. Cebra9, J. Ceska15, I. Chakaberia33, B. K. Chan10, Z. Chang27, A. Chatterjee16, D. Chen11, J. Chen49, J. H. Chen19, Z. Chen49, J. Cheng57, Y. Cheng10, S. Choudhury19, W. Christie6, X. Chu6, H. J. Crawford8, G. Dale-Gau13, A. Das15, A. P. Dash10, M. Daugherity1, T. G. Dedovich30, I. M. Deppner21, A. A. Derevschikov42, A. Dhamija41, P. Dixit24, X. Dong33, J. L. Drachenberg1, E. Duckworth31, J. C. Dunlop6, J. Engelage8, G. Eppley44, S. Esumi58, O. Evdokimov13, O. Eyser6, R. Fatemi32, S. Fazio7, C. J. Feng39, Y. Feng43, E. Finch51, Y. Fisyak6, F. A. Flor64, C. Fu28, T. Gao49, F. Geurts44, N. Ghimire54, A. Gibson60, K. Gopal25, X. Gou49, D. Grosnick60, A. Gupta29, A. Hamed4, Y. Han44, M. D. Harasty9, J. W. Harris64, H. Harrison-Smith32, W. He19, X. H. He28, Y. He49, C. Hu59, Q. Hu28, Y. Hu33, H. Huang39, H. Z. Huang10, S. L. Huang52, T. Huang13, X. Huang57, Y. Huang57, Y. Huang12, T. J. Humanic40, D. Isenhower1, M. Isshiki58, W. W. Jacobs27, A. Jalotra29, C. Jena25, Y. Ji33, J. Jia6,52, C. Jin44, X. Ju46, E. G. Judd8, S. Kabana53, D. Kalinkin32, K. Kang57, D. Kapukchyan11, K. Kauder6, D. Keane31, A. Kechechyan30, A. Kiselev6, A. G. Knospe34, H. S. Ko33, L. Kochenda37, A. A. Korobitsin30, A. Yu. Kraeva37, P. Kravtsov37, L. Kumar41, M. C. Labonte9, R. Lacey52, J. M. Landgraf6, A. Lebedev6, R. Lednicky30, J. H. Lee6, Y. H. Leung21, N. Lewis6, C. Li49, H-S. Li43, W. Li44, X. Li46, Y. Li46, Y. Li57, Z. Li46, X. Liang11, Y. Liang31, T. Lin49, Y. Lin20, C. Liu28, F. Liu12, G. Liu47, H. Liu12, L. Liu12, T. Liu64, X. Liu40, Y. Liu55, Z. Liu12, T. Ljubicic6, O. Lomicky15, R. S. Longacre6, E. M. Loyd11, T. Lu28, N. S. Lukow54, X. F. Luo12, V. B. Luong30, L. Ma19, R. Ma6, Y. G. Ma19, N. Magdy52, D. Mallick62, S. Margetis31, H. S. Matis33, G. McNamara63, K. Mi12, N. G. Minaev42, B. Mohanty38, M. M. Mondal38, I. Mooney64, D. A. Morozov42, A. Mudrokh30, M. I. Nagy17, A. S. Nain41, J. D. Nam54, M. Nasim24, E. Nedorezov30, D. Neff10, J. M. Nelson8, D. B. Nemes64, M. Nie49, G. Nigmatkulov13, T. Niida58, L. V. Nogach42, T. Nonaka58, G. Odyniec33, A. Ogawa6, S. Oh48, V. A. Okorokov37, K. Okubo58, B. S. Page6, R. Pak6, A. Pandav33, Y. Panebratsev30, T. Pani45, P. Parfenov37, A. Paul11, C. Perkins8, B. R. Pokhrel54, M. Posik54, A. Povarov37, T. Protzman34, N. K. Pruthi41, J. Putschke63, Z. Qin57, H. Qiu28, A. Quintero54, C. Racz11, S. K. Radhakrishnan31, A. Rana41, R. L. Ray56, H. G. Ritter33, C. W. Robertson43, O. V. Rogachevsky30, M. A. Rosales Aguilar32, D. Roy45, L. Ruan6, A. K. Sahoo24, N. R. Sahoo25, H. Sako58, S. Salur45, E. Samigullin2, S. Sato58, B. C. Schaefer34, W. B. Schmidke6,*, N. Schmitz35, J. Seger14, R. Seto11, P. Seyboth35, N. Shah26, E. Shahaliev30, P. V. Shanmuganathan6, T. Shao19, M. Sharma29, N. Sharma24, R. Sharma25, S. R. Sharma25, A. I. Sheikh31, D. Shen49, D. Y. Shen19, K. Shen46, S. S. Shi12, Y. Shi49, Q. Y. Shou19, F. Si46, J. Singh41, S. Singha28, P. Sinha25, M. J. Skoby5,43, Y. Söhngen21, Y. Song64, B. Srivastava43, T. D. S. Stanislaus60, D. J. Stewart63, M. Strikhanov37, B. Stringfellow43, Y. Su46, C. Sun52, X. Sun28, Y. Sun46, Y. Sun23, B. Surrow54, D. N. Svirida2, Z. W. Sweger9, A. C. Tamis64, A. H. Tang6, Z. Tang46, A. Taranenko37, T. Tarnowsky36, J. H. Thomas33, D. Tlusty14, T. Todoroki58, M. V. Tokarev30, S. Trentalange10, P. Tribedy6, S. K. Tripathy62, O. D. Tsai10,6, C. Y. Tsang31,6, Z. Tu6, J. Tyler55, T. Ullrich6, D. G. Underwood3,60, I. Upsal46, G. Van Buren6, A. N. Vasiliev42,37, V. Verkest63, F. Videbæk6, S. Vokal30, S. A. Voloshin63, F. Wang43, G. Wang10, J. S. Wang23, J. Wang49, X. Wang49, Y. Wang46, Y. Wang12, Y. Wang57, Z. Wang49, J. C. Webb6, P. C. Weidenkaff21, G. D. Westfall36, H. Wieman33, G. Wilks13, S. W. Wissink27, J. Wu12, J. Wu28, X. Wu10, X. Wu46, B. Xi19, Z. G. Xiao57, G. Xie59, W. Xie43, H. Xu23, N. Xu33, Q. H. Xu49, Y. Xu49, Y. Xu12, Z. Xu31, Z. Xu10, G. Yan49, Z. Yan52, C. Yang49, Q. Yang49, S. Yang47, Y. Yang39, Z. Ye44, Z. Ye33, L. Yi49, K. Yip6, Y. Yu49, W. Zha46, C. Zhang19, D. Zhang47, J. Zhang49, S. Zhang46, W. Zhang47, X. Zhang28, Y. Zhang28, Y. Zhang46, Y. Zhang49, Y. Zhang12, Z. J. Zhang39, Z. Zhang6, Z. Zhang13, F. Zhao28, J. Zhao19, M. Zhao6, C. Zhou19, J. Zhou46, S. Zhou12, Y. Zhou12, X. Zhu57, M. Zurek3,6, and M. Zyzak18 (STAR Collaboration)

  • 1Abilene Christian University, Abilene, Texas 79699
  • 2Alikhanov Institute for Theoretical and Experimental Physics NRC ”Kurchatov Institute,” Moscow 117218
  • 3Argonne National Laboratory, Argonne, Illinois 60439
  • 4American University in Cairo, New Cairo 11835, Egypt
  • 5Ball State University, Muncie, Indiana, 47306
  • 6Brookhaven National Laboratory, Upton, New York 11973
  • 7University of Calabria and INFN-Cosenza, Rende 87036, Italy
  • 8University of California, Berkeley, California 94720
  • 9University of California, Davis, California 95616
  • 10University of California, Los Angeles, California 90095
  • 11University of California, Riverside, California 92521
  • 12Central China Normal University, Wuhan, Hubei 430079
  • 13University of Illinois at Chicago, Chicago, Illinois 60607
  • 14Creighton University, Omaha, Nebraska 68178
  • 15Czech Technical University in Prague, FNSPE, Prague 115 19, Czech Republic
  • 16National Institute of Technology Durgapur, Durgapur-713209, India
  • 17ELTE Eötvös Loránd University, Budapest, Hungary H-1117
  • 18Frankfurt Institute for Advanced Studies FIAS, Frankfurt 60438, Germany
  • 19Fudan University, Shanghai, 200433
  • 20Guangxi Normal University, Guilin
  • 21University of Heidelberg, Heidelberg 69120, Germany
  • 22University of Houston, Houston, Texas 77204
  • 23Huzhou University, Huzhou, Zhejiang 313000
  • 24Indian Institute of Science Education and Research (IISER), Berhampur 760010, India
  • 25Indian Institute of Science Education and Research (IISER) Tirupati, Tirupati 517507, India
  • 26Indian Institute Technology, Patna, Bihar 801106, India
  • 27Indiana University, Bloomington, Indiana 47408
  • 28Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou, Gansu 730000
  • 29University of Jammu, Jammu 180001, India
  • 30Joint Institute for Nuclear Research, Dubna 141 980
  • 31Kent State University, Kent, Ohio 44242
  • 32University of Kentucky, Lexington, Kentucky 40506-0055
  • 33Lawrence Berkeley National Laboratory, Berkeley, California 94720
  • 34Lehigh University, Bethlehem, Pennsylvania 18015
  • 35Max-Planck-Institut für Physik, Munich 80805, Germany
  • 36Michigan State University, East Lansing, Michigan 48824
  • 37National Research Nuclear University MEPhI, Moscow 115409
  • 38National Institute of Science Education and Research, HBNI, Jatni 752050, India
  • 39National Cheng Kung University, Tainan 70101
  • 40The Ohio State University, Columbus, Ohio 43210
  • 41Panjab University, Chandigarh 160014, India
  • 42NRC ”Kurchatov Institute,” Institute of High Energy Physics, Protvino 142281
  • 43Purdue University, West Lafayette, Indiana 47907
  • 44Rice University, Houston, Texas 77251
  • 45Rutgers University, Piscataway, New Jersey 08854
  • 46University of Science and Technology of China, Hefei, Anhui 230026
  • 47South China Normal University, Guangzhou, Guangdong 510631
  • 48Sejong University, Seoul, 05006, South Korea
  • 49Shandong University, Qingdao, Shandong 266237
  • 50Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai 201800
  • 51Southern Connecticut State University, New Haven, Connecticut 06515
  • 52State University of New York, Stony Brook, New York 11794
  • 53Instituto de Alta Investigación, Universidad de Tarapacá, Arica 1000000, Chile
  • 54Temple University, Philadelphia, Pennsylvania 19122
  • 55Texas A&M University, College Station, Texas 77843
  • 56University of Texas, Austin, Texas 78712
  • 57Tsinghua University, Beijing 100084
  • 58University of Tsukuba, Tsukuba, Ibaraki 305-8571, Japan
  • 59University of Chinese Academy of Sciences, Beijing, 101408
  • 60Valparaiso University, Valparaiso, Indiana 46383
  • 61Variable Energy Cyclotron Centre, Kolkata 700064, India
  • 62Warsaw University of Technology, Warsaw 00-661, Poland
  • 63Wayne State University, Detroit, Michigan 48201
  • 64Yale University, New Haven, Connecticut 06520

  • *Deceased.

Phys. Rev. X 14, 011028 – Published 23 February, 2024

DOI: https://doi.org/10.1103/PhysRevX.14.011028

Abstract

The deconfined quark-gluon plasma (QGP) created in relativistic heavy-ion collisions enables the exploration of the fundamental properties of matter under extreme conditions. Noncentral collisions can produce strong magnetic fields on the order of 1018  G, which offers a probe into the electrical conductivity of the QGP. In particular, quarks and antiquarks carry opposite charges and receive contrary electromagnetic forces that alter their momenta. This phenomenon can be manifested in the collective motion of final-state particles, specifically in the rapidity-odd directed flow, denoted as v1(y). Here, we present the charge-dependent measurements of dv1/dy near midrapidities for π±, K±, and p(p¯) in Au+Au and isobar (Ru4496+Ru4496 and Zr4096+Zr4096) collisions at sNN=200  GeV, and in Au+Au collisions at 27 GeV, recorded by the STAR detector at the Relativistic Heavy Ion Collider. The combined dependence of the v1 signal on collision system, particle species, and collision centrality can be qualitatively and semiquantitatively understood as several effects on constituent quarks. While the results in central events can be explained by the u and d quarks transported from initial-state nuclei, those in peripheral events reveal the impacts of the electromagnetic field on the QGP. Our data put valuable constraints on the electrical conductivity of the QGP in theoretical calculations.

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Physics Subject Headings (PhySH)

Focus

Colossal Magnetic Field Detected in Nuclear Matter

Published 23 February, 2024

Collisions of heavy ions briefly produced a magnetic field 1018 times stronger than Earth’s, and it left observable effects.

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References (75)

  1. E. Shuryak, Strongly coupled quark-gluon plasma in heavy ion collisions, Rev. Mod. Phys. 89, 035001 (2017).
  2. E. W. Kolb and M. S. Turner, The Early Universe, Front. Phys. Vol. 69 (Westview Press, Boulder, 1990), p. 521.
  3. V. Voronyuk, V. D. Toneev, W. Cassing, E. L. Bratkovskaya, V. P. Konchakovski, and S. A. Voloshin, (Electro-)magnetic field evolution in relativistic heavy-ion collisions, Phys. Rev. C 83, 054911 (2011).
  4. W.-T. Deng and X.-G. Huang, Event-by-event generation of electromagnetic fields in heavy-ion collisions, Phys. Rev. C 85, 044907 (2012).
  5. X.-L. Zhao, G.-L. Ma, and Y.-G. Ma, Impact of magnetic-field fluctuations on measurements of the chiral magnetic effect in collisions of isobaric nuclei, Phys. Rev. C 99, 034903 (2019).
  6. D. E. Kharzeev, L. D. McLerran, and H. J. Warringa, The effects of topological charge change in heavy ion collisions: ‘Event by event P and CP violation’, Nucl. Phys. A803, 227 (2008).
  7. L. McLerran and V. Skokov, Comments about the electromagnetic field in heavy-ion collisions, Nucl. Phys. A929, 184 (2014).
  8. Z. Wang, J. Zhao, C. Greiner, Z. Xu, and P. Zhuang, Incomplete electromagnetic response of hot QCD matter, Phys. Rev. C 105, L041901 (2022).
  9. C. Grayson, M. Formanek, J. Rafelski, and B. Muller, Dynamic magnetic response of the quark-gluon plasma to electromagnetic fields, Phys. Rev. D 106, 014011 (2022).
  10. M. N. Chernodub, Superconductivity of QCD vacuum in strong magnetic field, Phys. Rev. D 82, 085011 (2010).
  11. I. E. Frolov, V. C. Zhukovsky, and K. G. Klimenko, Chiral density waves in quark matter within the Nambu-Jona-Lasinio model in an external magnetic field, Phys. Rev. D 82, 076002 (2010).
  12. M. N. Chernodub, Spontaneous electromagnetic superconductivity of vacuum in strong magnetic field: Evidence from the Nambu-Jona-Lasinio model, Phys. Rev. Lett. 106, 142003 (2011).
  13. Y. Burnier, D. E. Kharzeev, J. Liao, and H.-U. Yee, Chiral magnetic wave at finite baryon density and the electric quadrupole moment of quark-gluon plasma in heavy ion collisions, Phys. Rev. Lett. 107, 052303 (2011).
  14. X.-G. Huang, Electromagnetic fields and anomalous transports in heavy-ion collisions—A pedagogical review, Rep. Prog. Phys. 79, 076302 (2016).
  15. K. Hattori and X.-G. Huang, Novel quantum phenomena induced by strong magnetic fields in heavy-ion collisions, Nucl. Sci. Tech. 28, 26 (2017).
  16. D. E. Kharzeev and J. Liao, Chiral magnetic effect reveals the topology of gauge fields in heavy-ion collisions, Nat. Rev. Phys. 3, 55 (2021).
  17. K. Fukushima, D. E. Kharzeev, and H. J. Warringa, Chiral magnetic effect, Phys. Rev. D 78, 074033 (2008).
  18. D. E. Kharzeev, J. Liao, S. A. Voloshin, and G. Wang, Chiral magnetic and vortical effects in high-energy nuclear collisions—A status report, Prog. Part. Nucl. Phys. 88, 1 (2016).
  19. V. P. Gusynin, V. A. Miransky, and I. A. Shovkovy, Catalysis of dynamical flavor symmetry breaking by a magnetic field in (2+1)-dimensions, Phys. Rev. Lett. 73, 3499 (1994); 76, 1005(E) (1996).
  20. K. Tuchin, Synchrotron radiation by fast fermions in heavy-ion collisions, Phys. Rev. C 82, 034904 (2010); 83, 039903(E) (2011).
  21. A. J. Mizher, M. N. Chernodub, and E. S. Fraga, Phase diagram of hot QCD in an external magnetic field: Possible splitting of deconfinement and chiral transitions, Phys. Rev. D 82, 105016 (2010).
  22. R. K. Mohapatra, P. S. Saumia, and A. M. Srivastava, Enhancement of flow anisotropies due to magnetic field in relativistic heavy-ion collisions, Mod. Phys. Lett. A 26, 2477 (2011).
  23. K. Tuchin, On viscous flow and azimuthal anisotropy of quark-gluon plasma in strong magnetic field, J. Phys. G 39, 025010 (2012).
  24. S. K. Das, S. Plumari, S. Chatterjee, J. Alam, F. Scardina, and V. Greco, Directed flow of charm quarks as a witness of the initial strong magnetic field in ultra-relativistic heavy ion collisions, Phys. Lett. B 768, 260 (2017).
  25. A. Dubla, U. Gürsoy, and R. Snellings, Charge-dependent flow as evidence of strong electromagnetic fields in heavy-ion collisions, Mod. Phys. Lett. A 35, 2050324 (2020).
  26. U. Gürsoy, D. Kharzeev, E. Marcus, K. Rajagopal, and C. Shen, Charge-dependent flow induced by magnetic and electric fields in heavy ion collisions, Phys. Rev. C 98, 055201 (2018).
  27. U. Gursoy, D. Kharzeev, and K. Rajagopal, Magnetohydrodynamics, charged currents and directed flow in heavy ion collisions, Phys. Rev. C 89, 054905 (2014).
  28. K. Nakamura, T. Miyoshi, C. Nonaka, and H. R. Takahashi, Charge-dependent anisotropic flow in high-energy heavy-ion collisions from a relativistic resistive magneto-hydrodynamic expansion, Phys. Rev. C 107, 034912 (2023).
  29. L. Adamczyk et al. (STAR Collaboration), Charge-dependent directed flow in Cu+Au collisions at sNN=200  GeV, Phys. Rev. Lett. 118, 012301 (2017).
  30. L. Adamczyk et al. (STAR Collaboration), Azimuthal anisotropy in Cu+Au collisions at sNN=200  GeV, Phys. Rev. C 98, 014915 (2018).
  31. A. M. Poskanzer and S. A. Voloshin, Methods for analyzing anisotropic flow in relativistic nuclear collisions, Phys. Rev. C 58, 1671 (1998).
  32. S. A. Voloshin and T. Niida, Ultrarelativistic nuclear collisions: Direction of spectator flow, Phys. Rev. C 94, 021901(R) (2016).
  33. M. Luzum and J.-Y. Ollitrault, Directed flow at midrapidity in heavy-ion collisions, Phys. Rev. Lett. 106, 102301 (2011).
  34. U. Heinz and R. Snellings, Collective flow and viscosity in relativistic heavy-ion collisions, Annu. Rev. Nucl. Part. Sci. 63, 123 (2013).
  35. J. Adams et al. (STAR Collaboration), Directed flow in Au+Au collisions at sNN=62.4  GeV, Phys. Rev. C 73, 034903 (2006).
  36. B. I. Abelev et al. (STAR Collaboration), System-size independence of directed flow at the Relativistic Heavy-Ion Collider, Phys. Rev. Lett. 101, 252301 (2008).
  37. G. Agakishiev et al. (STAR Collaboration), Directed and elliptic flow of charged particles in Cu+Cu collisions at sNN=22.4  GeV, Phys. Rev. C 85, 014901 (2012).
  38. L. Adamczyk et al. (STAR Collaboration), Directed flow of identified particles in Au+Au collisions at sNN=200  GeV at RHIC, Phys. Rev. Lett. 108, 202301 (2012).
  39. L. Adamczyk et al. (STAR Collaboration), Beam-energy dependence of the directed flow of protons, antiprotons, and pions in Au+Au collisions, Phys. Rev. Lett. 112, 162301 (2014).
  40. L. Adamczyk et al. (STAR Collaboration), Beam-energy dependence of directed flow of Λ, Λ¯, K±, Ks0 and ϕ in Au+Au collisions, Phys. Rev. Lett. 120, 062301 (2018).
  41. J. Adam et al. (STAR Collaboration), First observation of the directed flow of D0 and D0¯ in Au+Au collisions at sNN=200  GeV, Phys. Rev. Lett. 123, 162301 (2019).
  42. J. Adam et al. (STAR Collaboration), Beam-energy dependence of the directed flow of deuterons in Au+Au collisions, Phys. Rev. C 102, 044906 (2020).
  43. B. Abelev et al. (ALICE Collaboration), Directed flow of charged particles at midrapidity relative to the spectator plane in Pb−Pb collisions at sNN=2.76  TeV, Phys. Rev. Lett. 111, 232302 (2013).
  44. In our notation, Δ(dv1/dy) is the dv1/dy difference between positively charged particles and their negatively charged antiparticles. For example, proton Δ(dv1/dy) means the dv1/dy difference between protons and antiprotons.

  45. D. Molnar and S. A. Voloshin, Elliptic flow at large transverse momenta from quark coalescence, Phys. Rev. Lett. 91, 092301 (2003).
  46. J. C. Dunlop, M. A. Lisa, and P. Sorensen, Constituent quark scaling violation due to baryon number transport, Phys. Rev. C 84, 044914 (2011).
  47. A. Goudarzi, G. Wang, and H. Z. Huang, Evidence of coalescence sum rule in elliptic flow of identified particles in high-energy heavy-ion collisions, Phys. Lett. B 811, 135974 (2020).
  48. R. C. Hwa and C. B. Yang, Scaling distributions of quarks, mesons, and proton for all pT, energy, and centrality, Phys. Rev. C 67, 064902 (2003).
  49. R. J. Fries, B. Müller, C. Nonaka, and S. A. Bass, Hadronization in heavy-ion collisions: Recombination and fragmentation of partons, Phys. Rev. Lett. 90, 202303 (2003).
  50. V. Greco, C. M. Ko, and P. Lévai, Parton coalescence and the antiproton/pion anomaly at RHIC, Phys. Rev. Lett. 90, 202302 (2003).
  51. S. Acharya et al. (ALICE Collaboration), Probing the effects of strong electromagnetic fields with charge-dependent directed flow in Pb−Pb collisions at the LHC, Phys. Rev. Lett. 125, 022301 (2020).
  52. Y. Guo, F. Liu, and A. Tang, Directed flow of transported and non-transported protons in Au+Au collisions from UrQMD model, Phys. Rev. C 86, 044901 (2012).
  53. K. Nayak, S. Shi, N. Xu, and Z.-W. Lin, Energy dependence study of directed flow in Au+Au collisions using an improved coalescence in a multiphase transport model, Phys. Rev. C 100, 054903 (2019).
  54. P. Bozek, Splitting of proton-antiproton directed flow in relativistic heavy-ion collisions, Phys. Rev. C 106, L061901 (2022).
  55. L. Adamczyk et al. (STAR Collaboration), Centrality dependence of identified particle elliptic flow in relativistic heavy ion collisions at sNN=7.7–62.4  GeV, Phys. Rev. C 93, 014907 (2016).
  56. M. Anderson et al., The STAR time projection chamber: A unique tool for studying high multiplicity events at RHIC, Nucl. Instrum. Methods Phys. Res., Sect. A 499, 659 (2003).
  57. W. Llope et al., The STAR vertex position detector, Nucl. Instrum. Methods Phys. Res., Sect. A 759, 23 (2014).
  58. M. L. Miller, K. Reygers, S. J. Sanders, and P. Steinberg, Glauber modeling in high energy nuclear collisions, Annu. Rev. Nucl. Part. Sci. 57, 205 (2007).
  59. B. I. Abelev et al. (STAR Collaboration), Systematic measurements of identified particle spectra in pp,d+ Au and Au+Au collisions from STAR, Phys. Rev. C 79, 034909 (2009).
  60. M. Abdallah et al. (STAR Collaboration), Search for the chiral magnetic effect with isobar collisions at sNN=200  GeV by the STAR Collaboration at the BNL Relativistic Heavy Ion Collider, Phys. Rev. C 105, 014901 (2022).
  61. W. Llope et al., The TOFp/pVPD time-of-flight system for star, Nucl. Instrum. Methods Phys. Res., Sect. A 522, 252 (2004).
  62. H. Bichsel, A method to improve tracking and particle identification in TPCs and silicon detectors, Nucl. Instrum. Methods Phys. Res., Sect. A 562, 154 (2006).
  63. C. Adler, A. Denisov, E. Garcia, M. Murray, H. Stroebele, and S. White, The RHIC zero degree calorimeters, Nucl. Instrum. Methods Phys. Res., Sect. A 470, 488 (2001).
  64. J. Adams et al., The STAR event plane detector, Nucl. Instrum. Methods Phys. Res., Sect. A 968, 163970 (2020).
  65. J. Barrette et al. (E877 Collaboration), Proton and pion production relative to the reaction plane in Au+Au collisions at 11  GeV/c, Phys. Rev. C 56, 3254 (1997).
  66. J. Brachmann, S. Soff, A. Dumitru, H. Stöcker, J. A. Maruhn, W. Greiner, L. V. Bravina, and D. H. Rischke, Antiflow of nucleons at the softest point of the equation of state, Phys. Rev. C 61, 024909 (2000).
  67. S. A. Bass et al., Microscopic models for ultrarelativistic heavy ion collisions, Prog. Part. Nucl. Phys. 41, 255 (1998).
  68. H. T. Ding, A. Francis, O. Kaczmarek, F. Karsch, E. Laermann, and W. Soeldner, Thermal dilepton rate and electrical conductivity: An analysis of vector current correlation functions in quenched lattice QCD, Phys. Rev. D 83, 034504 (2011).
  69. A. Francis and O. Kaczmarek, On the temperature dependence of the electrical conductivity in hot quenched lattice QCD, Prog. Part. Nucl. Phys. 67, 212 (2012).
  70. B. B. Brandt, A. Francis, H. B. Meyer, and H. Wittig, Thermal correlators in the ρ channel of two-flavor QCD, J. High Energy Phys. 3 (2013) 001.
  71. A. Amato, G. Aarts, C. Allton, P. Giudice, S. Hands, and J.-I. Skullerud, Electrical conductivity of the quark-gluon plasma across the deconfinement transition, Phys. Rev. Lett. 111, 172001 (2013).
  72. J. Balewski et al., Total cross section of the reaction pp→pK+Λ close to threshold, Phys. Lett. B 420, 211 (1998).
  73. T. Parida and S. Chatterjee, Baryon inhomogeneities driven charge dependent directed flow in heavy ion collisions, arXiv:2305.08806.
  74. J.-J. Zhang, X.-L. Sheng, S. Pu, J.-N. Chen, G.-L. Peng, J.-G. Wang, and Q. Wang, Charge-dependent directed flows in heavy-ion collisions by Boltzmann-Maxwell equations, Phys. Rev. Res. 4, 033138 (2022).
  75. STAR Collaboration, Electric charge and strangeness-dependent directed flow splitting of produced quarks in Au+Au collisions, arXiv:2304.02831.

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