meson production using a transport and a statistical hadronization model at energies covered by the RHIC beam energy scan
arXiv:2302.08177 · doi:10.1103/PhysRevC.108.044904
Abstract
In this paper, we discuss the centrality and energy dependence of resonance production using ultrarelativistic quantum molecular dynamics (UrQMD) and thermal models. The ratios obtained from the UrQMD and thermal models are compared with measurements done by the STAR experiment in Au+Au collisions at = 7.7, 11.5, 14.5, 19.6, 27, and 39 GeV. The ratio from the thermal model is consistent with data in most-peripheral collisions, however it overpredicts the ratio in central Au+Au collisions. This could be due to the fact that the thermal model does not have a hadronic rescattering phase, which is expected to be dominant in more central collisions. Furthermore, we have studied the ratio from UrQMD by varying the hadron propagation time () within the range 5 to 50 fm/c. It was found that the ratio decreases with increasing . Comparison between data and UrQMD suggest, one needs to consider a 10-50 fm/c to explain data at = 7.7-39 GeV in Au+Au collisions. We also predict the rapidity distribution of from UrQMD which could be measured in the STAR beam energy scan phase II (BES-II) program.
arXiv comment10 pages, 8 figures
References in corpus (34)
- Experimental and Theoretical Challenges in the Search for the Quark Gluon Plasma: The STAR Collaboration's Critical Assessment of the Evidence from RHIC Collisions
- Microscopic Models for Ultrarelativistic Heavy Ion Collisions
- Bulk Properties of the Medium Produced in Relativistic Heavy-Ion Collisions from the Beam Energy Scan Program
- Hadron production in Au-Au collisions at RHIC
- Thermal hadron production in pp and p{\bar p} collisions
- THERMUS -- A Thermal Model Package for ROOT
- K*(892) and (1020) production in Pb-Pb collisions at = 2.76 TeV
- K(892)* Resonance Production in Au+Au and p+p Collisions at sqrt(sNN) = 200 GeV at RHIC
- Strange Resonance Production: Probing Chemical and Thermal Freeze-out in Relativistic Heavy Ion Collisions
- Production of K(892) and (1020) in pp collisions at TeV
- K and meson production at high transverse momentum in pp and Pb-Pb collisions at = 2.76 TeV
- Hadronic resonance production and interaction in partonic and hadronic matter in EPOS3 with and without the hadronic afterburner UrQMD
- Hadron freeze-out conditions in high energy nuclear collisions
- Evidence of rescattering effect in Pb-Pb collisions at the LHC through production of and mesons
- K*0 production in Cu+Cu and Au+Au collisions at \sqrt{s_NN} = 62.4 GeV and 200 GeV
- Hadronic resonance production in +Au collisions at = 200 GeV at RHIC
- Production in Relativistic Heavy Ion Collisions at GeV
- Dynamics and freeze-out of hadron resonances at RHIC
- Sub-threshold and production by high mass resonances with UrQMD
- Influence of the hadronic phase on observables in ultrarelativistic heavy ion collisions
- Formation and decay of hadronic resonances in the QGP
- In-medium effects in strangeness production in heavy-ion collisions at (sub-)threshold energies
- and production in central Pb+Pb, Si+Si, C+C and inelastic p+p collisions at 158~GeV
- Production of K and in pp and Pb-Pb collisions at TeV
- Anti-strange meson-baryon interaction in hot and dense nuclear matter
- Measurement of and in , Au, and CuCu collisions at GeV
- Collision Broadening of the Phi Meson in Baryon Rich Hadronic Matter
- and production at midrapidity in pp collisions at = 8 TeV
- meson production in inelastic p+p interactions at 158 GeV/ beam momentum measured by NA61/SHINE at the CERN SPS
- production in Au+Au collisions at = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scan
- Studying re-scattering effect in heavy-ion collision through Production
- Medium effects on phi decays to dilepton and kaon-antikaon pairs in relativistic heavy ion reactions
- meson production in inelastic interactions at 40 and 80 GeV/ beam momenta measured by NA61/SHINE at the CERN SPS
- Upgrade of Hardware Controls for the STAR Experiment at RHIC