- Open Access
Examining hadronic resonance dynamics at energies available at the CERN Large Hadron Collider: Insights from EPOS4
Phys. Rev. C 113, 015202 – Published 21 January, 2026
DOI: https://doi.org/10.1103/ppg6-q16m
Abstract
Hadronic resonances, with lifetimes of a few are key tools for studying the hadronic phase in high-energy collisions. This work investigates resonance production in pp collisions at and in Pb-Pb collisions at using the EPOS4 model. The EPOS4 model provides the capability of switching the Ultrarelativistic Quantum Molecular Dynamics (UrQMD) ON or OFF, allowing the study of final-state hadronic interactions in the hadronic phase. Although this study is primarily focused on understanding the production of hadronic resonances, we also investigate the production of strange and nonstrange hadrons in relation to rescattering, regeneration, baryon-to-meson production, and strangeness enhancement, using transverse momentum () spectra and particle ratios. Rescattering effects and strangeness enhancement play an important role in the low- region, where soft, nonperturbative processes dominate particle production. At intermediate , the baryon-to-meson yield ratios show an enhancement, and the strong mass-dependent radial flow observed for baryons in the most central Pb-Pb collisions reflects the interplay between hadronization dynamics and collective effects. The average scaled with the reduced hadron mass (i.e., the mass divided by the number of valence quarks) is examined, revealing a deviation from a linear trend for short-lived resonances, attributed to hadronic phase effects. By analyzing the yield ratios of short-lived resonances to stable hadrons in pp and Pb-Pb collisions, the time duration () of the hadronic phase as a function of average charged multiplicity is estimated. The results show that increases with increasing multiplicity and system size, also exhibiting a nonzero value for high-multiplicity pp collisions. It is found that the production of baryons such as nonstrange (), strange (), and multistrange (, ) in the most central Pb-Pb collisions is influenced by competing processes of strangeness enhancement and baryon-antibaryon annihilation. Comparing these findings with measurements at energies available at the CERN Large Hadron Collider offers valuable insights into the underlying dynamics of the hadronic phase and their production dynamics.
Physics Subject Headings (PhySH)
Article Text
References (45)
- J. W. Harris and B. Müller, Annu. Rev. Nucl. Part. Sci. 46, 71 (1996).
- S. Acharya, et al. (ALICE Collaboration), Eur. Phys. J. C 84, 813 (2024).
- S. Acharya, et al. (ALICE Collaboration), Phys. Lett. B 807, 135501 (2020).
- S. Acharya, et al. (ALICE Collaboration), J. High Energy Phys. 05 (2024) 317.
- S. Acharya, et al. (ALICE Collaboration), Phys. Rev. C 99, 064901 (2019).
- S. Acharya, et al. (ALICE Collaboration), Eur. Phys. J. C 80, 160 (2020).
- S. Acharya, et al. (ALICE Collaboration), Phys. Lett. B 802, 135225 (2020).
- S. Acharya, et al. (ALICE Collaboration), Eur. Phys. J. C 83, 351 (2023).
- B. I. Abelev, et al. (STAR Collaboration), Phys. Rev. Lett. 97, 132301 (2006).
- J. Adams, et al. (STAR Collaboration), Phys. Rev. C 71, 064902 (2005).
- L. Gaudichet (STAR Collaboration), J. Phys. G 30, S549 (2004).
- S. Acharya, et al. (ALICE Collaboration), Phys. Rev. C 99, 024905 (2019).
- S. Acharya, et al. (ALICE Collaboration), Phys. Rev. C 106, 034907 (2022).
- S. Acharya, et al. (ALICE Collaboration), Phys. Rev. C 107, 055201 (2023).
- Z.-W. Lin, C. M. Ko, B.-A. Li, B. Zhang, and S. Pal, Phys. Rev. C 72, 064901 (2005).
- D. Oliinychenko and C. Shen, EPJ Web Conf. 259, 10008 (2022).
- A. Motornenko, V. Vovchenko, C. Greiner, and H. Stoecker, Phys. Rev. C 102, 024909 (2020).
- A. G. Knospe, C. Markert, K. Werner, J. Steinheimer, and M. Bleicher, Phys. Rev. C 104, 054907 (2021).
- A. G. Knospe, C. Markert, K. Werner, J. Steinheimer, and M. Bleicher, Phys. Rev. C 93, 014911 (2016).
- B. B. Abelev, et al. (ALICE Collaboration), Int. J. Mod. Phys. A 29, 1430044 (2014).
- K. Werner, Phys. Rev. C 109, 014910 (2024).
- V. N. Gribov, Zh. Eksp. Teor. Fiz. 53, 654 (1967) [Sov. Phys. JETP 26, 414 (1968)].
- V. N. Gribov, Zh. Eksp. Teor. Fiz. 56, 892 (1969) [Sov. Phys. JETP 29, 483 (1969)].
- V. N. Gribov and L. N. Lipatov, Sov. J. Nucl. Phys. 15, 438 (1972).
- V. A. Abramovsky, V. N. Gribov, and O. V. Kancheli, Yad. Fiz. 18, 595 (1973).
- G. Altarelli and G. Parisi, Nucl. Phys. B 126, 298 (1977).
- Y. L. Dokshitzer, Zh. Eksp. Teor. Fiz. 73, 1216 (1977) [Sov. Phys. JETP 46, 641 (1977)].
- L. V. Gribov, E. M. Levin, and M. G. Ryskin, Phys. Rep. 100, 1 (1983).
- L. D. McLerran and R. Venugopalan, Phys. Rev. D 49, 3352 (1994).
- L. D. McLerran and R. Venugopalan, Phys. Rev. D 49, 2233 (1994).
- A. Kovner, L. D. McLerran, and H. Weigert, Phys. Rev. D 52, 3809 (1995).
- Y. V. Kovchegov, Phys. Rev. D 54, 5463 (1996).
- T. Pierog, I. Karpenko, J. M. Katzy, E. Yatsenko, and K. Werner, Phys. Rev. C 92, 034906 (2015).
- K. Werner, Phys. Rev. Lett. 98, 152301 (2007).
- K. Werner, I. Karpenko, T. Pierog, M. Bleicher, and K. Mikhailov, Phys. Rev. C 82, 044904 (2010).
- K. Werner, B. Guiot, I. Karpenko, and T. Pierog, Phys. Rev. C 89, 064903 (2014).
- M. Bleicher, E. Zabrodin, C. Spieles, S. A. Bass, C. Ernst, S. Soff, L. Bravina, M. Belkacem, H. Weber, H Stöcker, and W. Greiner, J. Phys. G 25, 1859 (1999).
- S. Acharya, et al. (ALICE Collaboration), Phys. Rev. C 101, 044907 (2020).
- S. Acharya, et al. (ALICE Collaboration), Eur. Phys. J. C 81, 256 (2021).
- R. J. Fries, B. Muller, C. Nonaka, and S. A. Bass, Phys. Rev. Lett. 90, 202303 (2003).
- S. Acharya, et al. (ALICE Collaboration), Eur. Phys. J. C 80, 693 (2020).
- J. Adam, et al. (ALICE Collaboration), Eur. Phys. J. C 76, 245 (2016).
- S. Acharya, et al. (ALICE Collaboration), Eur. Phys. J. C 80, 167 (2020).
- B. B. Abelev, et al. (ALICE Collaboration), Phys. Rev. C 91, 024609 (2015).
- E. Seifert and W. Cassing, Phys. Rev. C 97, 024913 (2018).