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  • Open Access

QCD matter at a finite magnetic field and nonzero chemical potential

Zhi-Ying Qin1,2, Bo Feng1, Ya-Hui Hou1, Hong-Yue Song1, Wen-Chao Zhang1,*, Hua Zheng1, and Shi-Jun Mao3

  • *Contact author: wenchao.zhang@snnu.edu.cn

Phys. Rev. D 114, 016028 – Published 27 July, 2026

DOI: https://doi.org/10.1103/r8b2-3bnp

Abstract

We construct a hybrid equation of state (EoS) by smoothly interpolating the EoS in the hadron resonance gas at low temperatures to that in the ideal parton gas at high temperatures, and employ it to study the properties of the quantum chromodynamics (QCD) matter under a finite magnetic field and nonzero chemical potential. In this work, we neglect the anomalous magnetic moment effects of both charged and neutral particles. Our results show that the thermodynamic observables such as the entropy density, the pressure, the energy density, the trace anomaly, and the specific heat at constant volume are sensitive to both the finite magnetic field and chemical potential. As the chemical potential increases from zero, these quantities rise in both the hadronic and quark-gluon plasma phases. In contrast, introducing a magnetic field suppresses them at low temperatures but enhances them at high temperatures. Furthermore, nonzero chemical potential and magnetic field introduce nontrivial modifications to the squared speed of sound. Both effects increase its value near the critical temperature while reducing it at lower temperatures. When both the chemical potential and the magnetic field are present, their influences superimpose, leading to more intricate changes in the thermodynamic behavior. Finally, we compare our results with the lattice QCD data for the quadratic fluctuations of conserved charges and their correlations. The model successfully reproduces the temperature dependence of these observables at eB=0 and 0.04  GeV2. However, at the stronger field strength eB=0.14  GeV2, the model underestimates the magnitudes while still capturing the overall temperature trend.

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References (75)

  1. Y. Aoki, G. Endrodi, Z. Fodor, S. D. Katz, and K. K. Szabo, The order of the quantum chromodynamics transition predicted by the standard model of particle physics, Nature (London) 443, 675 (2006).
  2. S. Ejiri, Canonical partition function and finite density phase transition in lattice QCD, Phys. Rev. D 78, 074507 (2008).
  3. E. S. Bowman and J. I. Kapusta, Critical points in the linear sigma model with quarks, Phys. Rev. C 79, 015202 (2009).
  4. V. Skokov, A. Y. Illarionov, and V. Toneev, Estimate of the magnetic field strength in heavy-ion collisions, Int. J. Mod. Phys. A 24, 5925 (2009).
  5. W.-T. Deng and X.-G. Huang, Event-by-event generation of electromagnetic fields in heavy-ion collisions, Phys. Rev. C 85, 044907 (2012).
  6. J. O. Andersen, W. R. Naylor, and A. Tranberg, Phase diagram of QCD in a magnetic field, Rev. Mod. Phys. 88, 025001 (2016).
  7. V. A. Miransky and I. A. Shovkovy, Quantum field theory in a magnetic field: From quantum chromodynamics to graphene and Dirac semimetals, Phys. Rep. 576, 1 (2015).
  8. E. S. Fraga and L. F. Palhares, Deconfinement in the presence of a strong magnetic background: An exercise within the MIT bag model, Phys. Rev. D 86, 016008 (2012).
  9. V. D. Orlovsky and Y. A. Simonov, Quark-hadron thermodynamics in a magnetic field, Phys. Rev. D 89, 054012 (2014).
  10. X.-J. Wen and J. Zhang, Thermal effect in hot QCD matter in strong magnetic fields, Phys. Rev. C 109, 025203 (2024).
  11. M. Ruggieri, M. Tachibana, and V. Greco, Renormalized vs. nonrenormalized chiral transition in a magnetic background, J. High Energy Phys. 07 (2013) 165.
  12. J. O. Andersen, W. R. Naylor, and A. Tranberg, Inverse magnetic catalysis and regularization in the quark-meson model, J. High Energy Phys. 02 (2015) 042.
  13. X. Li, W.-j. Fu, and Y.-x. Liu, Thermodynamics of 2+1 flavor Polyakov-loop quark-meson model under external magnetic field, Phys. Rev. D 99, 074029 (2019).
  14. A. N. Tawfik and N. Magdy, SU(3) Polyakov linear-σ model in magnetic fields: Thermodynamics, higher-order moments, chiral phase structure, and meson masses, Phys. Rev. C 91, 015206 (2015).
  15. J. O. Andersen, W. R. Naylor, and A. Tranberg, Chiral and deconfinement transitions in a magnetic background using the functional renormalization group with the Polyakov loop, J. High Energy Phys. 04 (2014) 187.
  16. J. Zhang and X.-J. Wen, QCD phase transition with nonextensive NJL model in the strong magnetic field, Phys. Rev. D 110, 094049 (2024).
  17. R. He and X.-J. Wen, Effect of anomalous magnetic moment on the chiral transition at zero temperature in a strong magnetic field, Phys. Rev. D 106, 116023 (2022).
  18. S. Mao and S. Yang, Correlations and fluctuations in a magnetized three-flavor PNJL model with and without inverse magnetic catalysis effect, Phys. Rev. D 112, 014026 (2025).
  19. S. Mao, Reduction of pseudocritical temperatures of chiral restoration and deconfinement phase transitions in a magnetized PNJL model, Phys. Rev. D 110, 054002 (2024).
  20. S. Mao, Correlations and fluctuations in a magnetized PNJL model with and without the inverse magnetic catalysis effect, Chin. Phys. C 49, 063106 (2025).
  21. V. G. Bornyakov, P. V. Buividovich, N. Cundy, O. A. Kochetkov, and A. Schäfer, Deconfinement transition in two-flavor lattice QCD with dynamical overlap fermions in an external magnetic field, Phys. Rev. D 90, 034501 (2014).
  22. E.-M. Ilgenfritz, M. Muller-Preussker, B. Petersson, and A. Schreiber, Magnetic catalysis (and inverse catalysis) at finite temperature in two-color lattice QCD, Phys. Rev. D 89, 054512 (2014).
  23. H.-T. Ding, S.-T. Li, A. Tomiya, X.-D. Wang, and Y. Zhang, Chiral properties of (2+1)-flavor QCD in strong magnetic fields at zero temperature, Phys. Rev. D 104, 014505 (2021).
  24. H.-T. Ding, J.-B. Gu, A. Kumar, S.-T. Li, and J.-H. Liu, Baryon electric charge correlation as a magnetometer of QCD, Phys. Rev. Lett. 132, 201903 (2024).
  25. H.-T. Ding, J.-B. Gu, A. Kumar, and S.-T. Li, Second order fluctuations of conserved charges in external magnetic fields, Phys. Rev. D 111, 114522 (2025).
  26. N. Astrakhantsev, V. V. Braguta, A. Y. Kotov, and A. A. Roenko, QCD equation of state at nonzero baryon density in an external magnetic field, Phys. Rev. D 109, 094511 (2024).
  27. G. Endrödi, QCD equation of state at nonzero magnetic fields in the hadron resonance gas model, J. High Energy Phys. 04 (2013) 023.
  28. V. Vovchenko, Magnetic field effect on hadron yield ratios and fluctuations in a hadron resonance gas, Phys. Rev. C 110, 034914 (2024).
  29. E. S. Fraga, L. F. Palhares, and T. E. Restrepo, Cold and dense perturbative QCD in a very strong magnetic background, Phys. Rev. D 109, 054033 (2024).
  30. M. Asakawa, U. W. Heinz, and B. Muller, Fluctuation probes of quark deconfinement, Phys. Rev. Lett. 85, 2072 (2000).
  31. S. Jeon and V. Koch, Charged particle ratio fluctuation as a signal for quark-gluon plasma, Phys. Rev. Lett. 85, 2076 (2000).
  32. S. Ejiri, F. Karsch, and K. Redlich, Hadronic fluctuations at the QCD phase transition, Phys. Lett. B 633, 275 (2006).
  33. X. Luo and N. Xu, Search for the QCD critical point with fluctuations of conserved quantities in relativistic heavy-ion collisions at RHIC: An overview, Nucl. Sci. Tech. 28, 112 (2017).
  34. M. A. Stephanov, On the sign of kurtosis near the QCD critical point, Phys. Rev. Lett. 107, 052301 (2011).
  35. J. Adam et al. (STAR Collaboration), Nonmonotonic energy dependence of net-proton number fluctuations, Phys. Rev. Lett. 126, 092301 (2021).
  36. M. Abdallah et al. (STAR Collaboration), Cumulants and correlation functions of net-proton, proton, and antiproton multiplicity distributions in Au+Au collisions at energies available at the BNL Relativistic Heavy Ion Collider, Phys. Rev. C 104, 024902 (2021).
  37. M. Ferreira, P. Costa, and C. Providência, Net baryon-number fluctuations in magnetized quark matter, Phys. Rev. D 98, 034003 (2018).
  38. W.-j. Fu, Fluctuations and correlations of hot QCD matter in an external magnetic field, Phys. Rev. D 88, 014009 (2013).
  39. H.-T. Ding, S.-T. Li, Q. Shi, and X.-D. Wang, Fluctuations and correlations of net baryon number, electric charge and strangeness in a background magnetic field, Eur. Phys. J. A 57, 202 (2021).
  40. M. Marczenko, M. Szymański, P. M. Lo, B. Karmakar, P. Huovinen, C. Sasaki, and K. Redlich, Magnetic effects in the hadron resonance gas, Phys. Rev. C 110, 065203 (2024).
  41. A. Bhattacharyya, S. K. Ghosh, R. Ray, and S. Samanta, Exploring effects of magnetic field on the hadron resonance gas, Europhys. Lett. 115, 62003 (2016).
  42. K. Fukushima and Y. Hidaka, Magnetic shift of the chemical freeze-out and electric charge fluctuations, Phys. Rev. Lett. 117, 102301 (2016).
  43. G. Kadam, S. Pal, and A. Bhattacharyya, Interacting hadron resonance gas model in magnetic field and the fluctuations of conserved charges, J. Phys. G 47, 125106 (2020).
  44. E. S. Fraga, L. F. Palhares, and T. E. Restrepo, Susceptibilities and Taylor coefficients of magnetic QCD from perturbation theory, Phys. Rev. D 113, 014014 (2026).
  45. S. Borsanyi, G. Endrodi, Z. Fodor, A. Jakovac, S. D. Katz, S. Krieg, C. Ratti, and K. K. Szabo, The QCD equation of state with dynamical quarks, J. High Energy Phys. 11 (2010) 077.
  46. A. Bazavov et al. (HotQCD Collaboration), Equation of state in (2+1)-flavor QCD, Phys. Rev. D 90, 094503 (2014).
  47. D. Bollweg, J. Goswami, O. Kaczmarek, F. Karsch, S. Mukherjee, P. Petreczky, C. Schmidt, and P. Scior (HotQCD Collaboration), Second order cumulants of conserved charge fluctuations revisited: Vanishing chemical potentials, Phys. Rev. D 104, 074512 (2021).
  48. F. Karsch, K. Redlich, and A. Tawfik, Thermodynamics at nonzero baryon number density: A Comparison of lattice and hadron resonance gas model calculations, Phys. Lett. B 571, 67 (2003).
  49. A. Tawfik, QCD phase diagram: A Comparison of lattice and hadron resonance gas model calculations, Phys. Rev. D 71, 054502 (2005).
  50. C. R. Allton, M. Doering, S. Ejiri, S. J. Hands, O. Kaczmarek, F. Karsch, E. Laermann, and K. Redlich, Thermodynamics of two flavor QCD to sixth order in quark chemical potential, Phys. Rev. D 71, 054508 (2005).
  51. J. Kapusta and C. Gale, Finite temperature Field Theory: Principles and Applications, Cambridge Monographs on Mathematical Physics (Cambridge University Press, Cambridge, England, 2006).
  52. M. Asakawa and T. Hatsuda, What thermodynamics tells about QCD plasma near phase transition, Phys. Rev. D 55, 4488 (1997).
  53. K. Kyan and A. Monnai, QCD equation of state with Tsallis statistics for heavy-ion collisions, Phys. Rev. D 106, 054004 (2022).
  54. J.-H. Shi, Z.-Y. Qin, J.-P. Zhang, J. Cao, Z.-F. Jiang, W.-C. Zhang, and H. Zheng, Nonextensive (3+1)-dimensional hydrodynamics for relativistic heavy-ion collisions, Phys. Rev. D 111, 036010 (2025).
  55. A. Bazavov et al. (HotQCD Collaboration), Fluctuations and correlations of net baryon number, electric charge, and strangeness: A comparison of lattice QCD results with the hadron resonance gas model, Phys. Rev. D 86, 034509 (2012).
  56. M. Cheng, P. Hegde, C. Jung, F. Karsch, O. Kaczmarek, E. Laermann, R. D. Mawhinney, C. Miao, P. Petreczky, C. Schmidt, and W. Soeldner, Baryon number, strangeness and electric charge fluctuations in QCD at high temperature, Phys. Rev. D 79, 074505 (2009).
  57. V. Dexheimer, D. P. Menezes, and M. Strickland, The influence of strong magnetic fields on proto-quark stars, J. Phys. G 41, 015203 (2014).
  58. L. Landau and E. Lifshitz, Quantum Mechanics: Non-Relativistic Theory, Course of Theoretical Physics, Vol. 3 (Pergamon, Oxford, 1977).
  59. G. S. Bali, F. Bruckmann, G. Endrodi, Z. Fodor, S. D. Katz, S. Krieg, A. Schafer, and K. K. Szabo, The QCD phase diagram for external magnetic fields, J. High Energy Phys. 02 (2012) 044.
  60. S. Gupta, X. Luo, B. Mohanty, H. G. Ritter, and N. Xu, Scale for the phase diagram of quantum chromodynamics, Science 332, 1525 (2011).
  61. 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).
  62. N. Sharma, J. Cleymans, B. Hippolyte, and M. Paradza, Comparison of p−p, p−Pb, and Pb−Pb collisions in the thermal model: Multiplicity dependence of thermal parameters, Phys. Rev. C 99, 044914 (2019).
  63. S. Durr, Z. Fodor, C. Hoelbling, S. D. Katz, S. Krieg, T. Kurth, L. Lellouch, T. Lippert, K. K. Szabo, and G. Vulvert (BMW Collaboration), Lattice QCD at the physical point: Light quark masses, Phys. Lett. B 701, 265 (2011).
  64. C. Patrignani et al. (Particle Data Group), Review of particle physics, Chin. Phys. C 40, 100001 (2016).
  65. A. Bazavov et al. (HotQCD Collaboration), Chiral crossover in QCD at zero and non-zero chemical potentials, Phys. Lett. B 795, 15 (2019).
  66. E. S. Fraga, L. F. Palhares, and T. E. Restrepo, Hot perturbative QCD in a very strong magnetic background, Phys. Rev. D 108, 034026 (2023).
  67. K. Kajantie, M. Laine, K. Rummukainen, and Y. Schröder, Pressure of hot QCD up to g6ln(1/g), Phys. Rev. D 67, 105008 (2003).
  68. V. Skokov, A. Yu. Illarionov, and V. Toneev, Estimate of the magnetic field strength in heavy-ion collisions, Int. J. Mod. Phys. A 24, 5925 (2009).
  69. L. Adamczyk et al. (STAR Collaboration), Bulk properties of the medium produced in relativistic heavy-ion collisions from the beam energy scan program, Phys. Rev. C 96, 044904 (2017).
  70. D. Atta, N. Chaudhuri, and S. Ghosh, Finite size effect on the thermodynamics of a hot and magnetized hadron resonance gas, Mod. Phys. Lett. A 37, 2250211 (2022).
  71. F. Gao, J. Chen, Y.-X. Liu, S.-X. Qin, C. D. Roberts, and S. M. Schmidt, Phase diagram and thermal properties of strong-interaction matter, Phys. Rev. D 93, 094019 (2016).
  72. Z.-Y. Qin, J.-H. Shi, J.-P. Zhang, J. Cao, B. Feng, W.-C. Zhang, H. Zheng, and S.-J. Mao, QCD phase transition at finite temperature and chemical potential with nonextensive statistics, Phys. Rev. D 112, 096022 (2025).
  73. A. Vuorinen, Quark number susceptibilities of hot QCD up to g6ln(1/g), Phys. Rev. D 67, 074032 (2003).
  74. R. Samanta and W. Broniowski, Magnetic properties of the hadron resonance gas with physical magnetic moments, Phys. Rev. C 112, 045202 (2025).
  75. P. Petreczky, Lattice QCD at non-zero temperature. J. Phys. G 39, 093002 (2012).

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