Reuse & Permissions

It is not necessary to obtain permission to reuse this article or its components as it is available under the terms of the Creative Commons Attribution 4.0 International license. This license permits unrestricted use, distribution, and reproduction in any medium, provided attribution to the author(s) and the published article's title, journal citation, and DOI are maintained. Please note that some figures may have been included with permission from other third parties. It is your responsibility to obtain the proper permission from the rights holder directly for these figures.

Export citation

Export citation

Choose format for download:

Download Citation
  • Open Access

Temperature dependence of the masses of various meson states: A comparative study in the SU(3) and SU(4) extended linear-σ models

A. Friesen1, Yu. Kalinovsky1, S. O. Allehabi2, N. M. Rfeek3, A. A. Alshehri4, and A. Tawfik2,*

  • *Contact author: tawfik@itp.uni-frankfurt.de, 400778@iu.edu.sa, atawfik@bnl.gov

Phys. Rev. C 114, 015207 – Published 27 July, 2026

DOI: https://doi.org/10.1103/ms99-5qnq

Abstract

In the extended Linear-σ Model (eLSM), the chiral phase structure of meson states, including pseudoscalars (Jpc=0−+), scalars (Jpc=0++), vectors (Jpc=1−−), and axial vectors (Jpc=1++), is investigated with the mean-field approximation. A systematic comparison between SU(3) and SU(4) configurations is provided. It has been found that the estimations of meson masses derived from SU(4) eLSM are more congruent with experimental values than those derived from SU(3) eLSM. Consequently, we conclude that an increase in quark degrees of freedom significantly enhances the accuracy of meson mass simulations. We investigate the effect of temperature on the masses of various meson states calculated in the SU(3) and SU(4) eLSM. After establishing all the fitting parameters, the temperature dependence of meson masses shows that although various meson states exhibit unique patterns in their mass changes with temperature, they all seem to share a similar range of dissolution temperatures. This means that the critical temperature that marks the phase transition from hadrons to quarks appears to vary slightly depending on the meson states. In this regard, we find that the quarkonium states, formed by a quark and its antiquark, are largely unaffected by variations in the temperature.

View figure in article

Physics Subject Headings (PhySH)

Article Text

References (79)

  1. A. Tawfik, N. Magdy, and A. Diab, Polyakov linear SU(3) sigma model: Features of higher-order moments in a dense and thermal hadronic medium, Phys. Rev. C 89, 055210 (2014).
  2. A. N. Tawfik, A. M. Diab, N. Ezzelarab, and A. G. Shalaby, QCD thermodynamics and magnetization in nonzero magnetic field, Adv. High Energy Phys. 2016, 1381479 (2016).
  3. A. N. Tawfik, A. M. Diab, and M. T. Hussein, Quark–hadron phase structure, thermodynamics, and magnetization of QCD matter, J. Phys. G: Nucl. Part. Phys. 45, 055008 (2018).
  4. A. N. Tawfik, A. M. Diab, and M. T. Hussein, SU(3) Polyakov linear-sigma model: Conductivity and viscous properties of QCD matter in thermal medium, Int. J. Mod. Phys. A 31, 1650175 (2016).
  5. H. Pagels, Dynamical chiral symmetry breaking in quantum chromodynamics, Phys. Rev. D 19, 3080 (1979).
  6. S. Gasiorowicz and D. A. Geffen, Effective Lagrangians and field algebras with chiral symmetry, Rev. Mod. Phys. 41, 531 (1969).
  7. C. Becchi, S. Narison, E. de Rafael, and F. J. Yndurain, Light quark masses in quantum chromodynamics and chiral symmetry breaking, Z. Phys. C 8, 335 (1981).
  8. T. L. Trueman, Chiral symmetry in perturbative QCD, Phys. Lett. B 88, 331 (1979).
  9. A. A. Osipov, B. Hiller, and A. H. Blin, Effective multiquark interactions with explicit breaking of chiral symmetry, Phys. Rev. D 88, 054032 (2013).
  10. K. Freese, J. A. Frieman, and A. V. Olinto, Natural inflation with pseudo–Nambu-Goldstone bosons, Phys. Rev. Lett. 65, 3233 (1990).
  11. R. Foot, A. Kobakhidze, and R. R. Volkas, Electroweak Higgs as a pseudo-Goldstone boson of broken scale invariance, Phys. Lett. B 655, 156 (2007).
  12. K. Yamada, M. Ishida, S. Ishida, D. Ito, T. Komada, and H. Tonooka, Possible evidence for a chiral axial vector state in the D meson system, AIP Conf. Proc. 619, 657 (2002).
  13. D. J. Wilson, C. E. Thomas, J. J. Dudek, and R. G. Edwards, Charmonium χc0 and χc2 resonances in coupled-channel scattering from lattice QCD, Phys. Rev. D 109, 114503 (2024).
  14. R. G. Jafarov and V. E. Rochev, Mean field expansion and meson effects in chiral condensate of analytically regularized Nambu-Jona-Lasinio model, Central Eur. J. Phys. 2, 367 (2004).
  15. M. Matsuo and T. Matsui, Quantized meson fields in and out of equilibrium. II: Chiral condensate and collective meson excitations, arXiv:0812.1853.
  16. Z. Zhang, C. Shi, and H.-S. Zong, Nambu–Jona-Lasinio model in a sphere, Phys. Rev. D 101, 043006 (2020).
  17. C. S. Fischer, QCD at finite temperature and chemical potential from Dyson–Schwinger equations, Prog. Part. Nucl. Phys. 105, 1 (2019).
  18. A. Ayala, A. Bashir, C. A. Dominguez, E. Gutierrez, M. Loewe, and A. Raya, QCD phase diagram from finite energy sum rules, Phys. Rev. D 84, 056004 (2011).
  19. D. Espriu, N. Gómez, and A. Vioque-Rodríguez, Chiral perturbation theory for nonzero chiral imbalance, J. High Energy Phys. 06 (2020) 062.
  20. F. Karsch, K. Redlich, and A. Tawfik, Hadron resonance mass spectrum and lattice QCD thermodynamics, Eur. Phys. J. C 29, 549 (2003).
  21. 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).
  22. Y.-P. Zhao, Thermodynamic properties and transport coefficients of QCD matter within the nonextensive Polyakov–Nambu–Jona-Lasinio model, Phys. Rev. D 101, 096006 (2020).
  23. M. Buballa, NJL model analysis of quark matter at large density, Phys. Rep. 407, 205 (2005).
  24. A. N. Tawfik and A. M. Diab, Polyakov SU(3) extended linear-σ model: Sixteen mesonic states in chiral phase structure, Phys. Rev. C 91, 015204 (2015).
  25. A. N. Tawfik, A. M. Diab, and M. T. Hussein, Chiral phase structure of the sixteen meson states in the SU(3) Polyakov linear-sigma model for finite temperature and chemical potential in a strong magnetic field, Chin. Phys. C 43, 034103 (2019).
  26. S. Gallas, F. Giacosa, and D. H. Rischke, Vacuum phenomenology of the chiral partner of the nucleon in a linear sigma model with vector mesons, Phys. Rev. D 82, 014004 (2010).
  27. D. Parganlija, F. Giacosa, and D. H. Rischke, Vacuum properties of mesons in a linear sigma model with vector mesons and global chiral invariance, Phys. Rev. D 82, 054024 (2010).
  28. S. Janowski, D. Parganlija, F. Giacosa, and D. H. Rischke, The glueball in a chiral linear sigma model with vector mesons, Phys. Rev. D 84, 054007 (2011).
  29. S. Narison, Light and heavy quark masses, test of PCAC and flavor breakings of condensates in QCD, Phys. Lett. B 216, 191 (1989).
  30. G. 't Hooft, Symmetry breaking through Bell-Jackiw anomalies, Phys. Rev. Lett. 37, 8 (1976).
  31. D. Parganlija, P. Kovacs, G. Wolf, F. Giacosa, and D. H. Rischke, Meson vacuum phenomenology in a three-flavor linear sigma model with (axial-)vector mesons, Phys. Rev. D 87, 014011 (2013).
  32. A. N. Tawfik, A. I. Ahmadov, A. Friesen, Y. Kalinovsky, A. Aparin, and M. Hanafy, Derivation of meson masses in SU(3) and SU(4) extended linear sigma model at finite temperature, Particles 8, 9 (2025).
  33. R. Vertesi, T. Csorgo, and J. Sziklai, Significant in-medium η′ mass reduction in sNN=200 GeV Au+Au collisions at the BNL Relativistic Heavy Ion Collider, Phys. Rev. C 83, 054903 (2011).
  34. W. Cassing, Transport analysis of in-medium hadron effects in pA and AA collisions, Eur. Phys. J. A 18, 467 (2003).
  35. A. Dainese, Perspectives for the study of charm in-medium quenching at the LHC with ALICE, Eur. Phys. J. C 33, 495 (2004).
  36. A. Tawfik, In-medium modifications of hadron properties, Indian J. Phys. 85, 755 (2011).
  37. J. Friese, Studying in-medium hadron properties with HADES, Prog. Part. Nucl. Phys. 42, 235 (1999).
  38. L. Tolos, J. Schaffner-Bielich, and H. Stoecker, D-mesons: In-medium effects at FAIR, Phys. Lett. B 635, 85 (2006).
  39. D. Finogeev, M. Golubeva, F. Guber, A. Ivashkin, A. Izvestnyy, N. Karpushkin, S. Morozov, and A. Reshetin, The PSD CBM supermodule response study for hadrons in momentum range 2 – 6 GeV/c at CERN test beams, KnE Energ. Phys. 3, 333 (2018).
  40. P. Parfenov, D. Idrisov, V. B. Luong, N. Geraksiev, A. Truttse, and A. Demanov, Anisotropic flow measurements of identified hadrons with MPD detector at NICA, Particles 4, 146 (2021).
  41. F. Giacosa, D. Parganlija, P. Kovacs, and G. Wolf, Phenomenology of light mesons within a chiral approach, EPJ Web Conf. 37, 08006 (2012).
  42. R. D. Pisarski and F. Rennecke, Conjectures about the chiral phase transition in QCD from anomalous multi-instanton interactions, Phys. Rev. Lett. 132, 251903 (2024).
  43. F. Giacosa, G. Kovács, P. Kovács, R. D. Pisarski, and F. Rennecke, Anomalous U(1)A couplings and the Columbia plot, Phys. Rev. D 111, 016014 (2025).
  44. J. Meyer, K. Schwenzer, H.-J. Pirner, and A. Deandrea, Renormalization group flow in large Nc, Phys. Lett. B 526, 79 (2002).
  45. A. Heinz, Phenomenological improvement of the linear-σ model in the large-Nc limit, Acta Phys. Pol. B Proc. Suppl. 4, 561 (2011).
  46. A. Heinz, F. Giacosa, and D. H. Rischke, Restoration of chiral symmetry in the large-Nc limit, Phys. Rev. D 85, 056005 (2012).
  47. J. Gasser and H. Leutwyler, Light quarks at low temperatures, Phys. Lett. B 184, 83 (1987).
  48. P. Kovács, Z. Szép, and G. Wolf, Existence of the critical endpoint in the vector meson extended linear sigma model, Phys. Rev. D 93, 114014 (2016).
  49. J. A. Mignaco and E. Remiddi, On the renormalization of the linear sigma-model, Nuovo Cimento A 1, 376 (1971).
  50. C. Contreras and M. Loewe, The linear σ model and finite temperature effects, Int. J. Mod. Phys. A 05, 2297 (1990).
  51. A. Bhattacharyya and S. Raha, Temperature dependence of hadron masses: I. Results from an extended linear sigma model, J. Phys. G: Nucl. Part. Phys. 21, 741 (1995).
  52. H.-S. Roh and T. Matsui, Chiral phase transition at finite temperature in the linear sigma model, Eur. Phys. J. A 1, 205 (1998).
  53. R. Delbourgo and M. D. Scadron, Dynamical generation of linear sigma model SU(3) Lagrangian and meson nonet mixing, Int. J. Mod. Phys. A 13, 657 (1998).
  54. J. T. Lenaghan, D. H. Rischke, and J. Schaffner-Bielich, Chiral symmetry restoration at nonzero temperature in the SU(3)r×SU(3)l linear sigma model, Phys. Rev. D 62, 085008 (2000).
  55. A. I. Ahmadov, A. A. Alshehri, and A. N. Tawfik, Mass spectrum of non-charmed and charmed meson states in extended linear-sigma model, Particles 7, 560 (2024).
  56. R. E. Mott, SU(4) × SU(4) symmetry breaking and its implications for SU(3) × SU(3) breaking, Nucl. Phys. B 84, 260 (1975).
  57. J. C. Myers and M. C. Ogilvie, New phases of SU(3) and SU(4) at finite temperature, Phys. Rev. D 77, 125030 (2008).
  58. A. N. Tawfik, C. Greiner, A. M. Diab, M. T. Ghoneim, and H. Anwer, Polyakov linear-σ model in mean-field approximation and optimized perturbation theory, Phys. Rev. C 101, 035210 (2020).
  59. B.-J. Schaefer and M. Wagner, The three-flavor chiral phase structure in hot and dense QCD matter, Phys. Rev. D 79, 014018 (2009).
  60. B.-J. Schaefer and J. Wambach, Susceptibilities near the QCD (tri)critical point, Phys. Rev. D 75, 085015 (2007).
  61. O. Scavenius, A. Mocsy, I. N. Mishustin, and D. H. Rischke, Chiral phase transition within effective models with constituent quarks, Phys. Rev. C 64, 045202 (2001).
  62. M. Cheng et al., The QCD equation of state with almost physical quark masses, Phys. Rev. D 77, 014511 (2008).
  63. J. I. Kapusta and C. Gale, Finite-Temperature Field Theory: Principles and Applications (Cambridge University Press, Cambridge, 2011).
  64. A. N. Tawfik, A. M. Diab, M. T. Ghoneim, and H. Anwer, SU(3) Polyakov linear-sigma model with finite isospin asymmetry: QCD phase diagram, Int. J. Mod. Phys. A 34, 1950199 (2019).
  65. A. N. Tawfik and A. M. Diab, Chiral magnetic properties of QCD phase-diagram, Eur. Phys. J. A 57, 200 (2021).
  66. U. S. Gupta and V. K. Tiwari, Meson masses and mixing angles in 2+1 flavor Polyakov quark meson sigma model and symmetry restoration effects, Phys. Rev. D 81, 054019 (2010).
  67. A. M. Diab, Charmed meson structure across crossover from SU(4) Polyakov quark meson model with isospin asymmetry, Chin. Phys. C 50, 013101 (2026).
  68. W. I. Eshraim, F. Giacosa, and D. H. Rischke, Phenomenology of charmed mesons in the extended linear sigma model, Eur. Phys. J. A 51, 112 (2015).
  69. R. V. Gavai, M. E. Jaensch, O. Kaczmarek, F. Karsch, M. Sarkar, R. Shanker, S. Sharma, S. Sharma, and T. Ueding, Aspects of the chiral crossover transition in (2+1)-flavor QCD with Möbius domain-wall fermions, Phys. Rev. D 111, 034507 (2025).
  70. B.-J. Schaefer, J. M. Pawlowski, and J. Wambach, The phase structure of the Polyakov–quark-meson model, Phys. Rev. D 76, 074023 (2007).
  71. A. Friesen, Y. Kalinovsky, and V. Toneev, Phase diagram in the entanglement PNJL model, J. Phys.: Conf. Ser. 668, 012128 (2016).
  72. S. Navas et al., Review of particle physics, Phys. Rev. D 110, 030001 (2024).
  73. D. Parganlija, P. Kovacs, G. Wolf, F. Giacosa, and D. H. Rischke, Scalar mesons in a linear sigma model with (axial-) vector mesons, AIP Conf. Proc. 1520, 226 (2013).
  74. T. Feldmann, P. Kroll, and B. Stech, Mixing and decay constants of pseudoscalar mesons, Phys. Rev. D 58, 114006 (1998).
  75. C. Di Donato, G. Ricciardi, I. Bigi, η−η′ mixing: From electromagnetic transitions to weak decays of charm and beauty hadrons, Phys. Rev. D 85, 013016 (2012).
  76. E. Klempt, Glueballs, hybrids, pentaquarks: Introduction to hadron spectroscopy and review of selected topics, presented at the 18th Annual Hampton University Graduate Studies Program, Jefferson Lab, Newport News, Virginia, June 2–20, 2003 (unpublished).
  77. B. Bagchi, P. Bhattacharyya, S. Sen, and J. Chakrabarti, Mixing angles and decay constants of η,η′, and ηc, Phys. Rev. D 60, 074002 (1999).
  78. H. Navelet, The B+,D+,Ds+ mixing angles and SU(4), Z. Phys. C 5, 325 (1980).
  79. Y.-J. Zhang, X.-G. Wu, D.-D. Hu, and L. Zeng, η−η′ mixing and its application in the B+,D+,Ds+→η(′)ℓ+νℓ decays, Phys. Rev. D 112, 076001 (2025).

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation