L. Bravina, Yu. Kvasiuk, D. Sachenko, S. Sivoklokov, O. Vitiuk, E. Zabrodin
{"title":"Directed flow and freeze-out in relativistic heavy-ion collisions at NICA and FAIR energies","authors":"L. Bravina, Yu. Kvasiuk, D. Sachenko, S. Sivoklokov, O. Vitiuk, E. Zabrodin","doi":"10.22323/1.347.0171","DOIUrl":null,"url":null,"abstract":"Directed flow of charged particles is studied in \nnucleus-nucleus collisions simulated within the energy range accessible \nfor NICA and FAIR facilities. Two transport cascade models, UrQMD and \nQGSM, are employed. These models use different mechanisms of the string \nexcitation and string fragmentation. Despite of the differences, \ndirected flows of charged pions and charged kaons in both models remain \nantiflow-oriented with reduction of the collision energy from $\\sqrt{s} \n= 11.5$~GeV to 3.5~GeV. In contrast, the directed flow of protons \nchanges its sign from antiflow to normal flow within the investigated \nenergy interval. Both models favor continuous non-uniform emittence of \nhadrons from the expanding fireball rather than sharp, or sudden, \nfreeze-out picture adopted by majority of hydrodynamic models. We found \nthat the earlier frozen hadrons carry the strongest directed flow at \nmidrapidity, although the flow development even at $|y| \\leq 0.5$ takes \nabout 8-12~fm/$c$ for different hadron species.","PeriodicalId":278184,"journal":{"name":"Proceedings of Corfu Summer Institute 2018 \"School and Workshops on Elementary Particle Physics and Gravity\" — PoS(CORFU2018)","volume":"83 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2019-09-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proceedings of Corfu Summer Institute 2018 \"School and Workshops on Elementary Particle Physics and Gravity\" — PoS(CORFU2018)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.22323/1.347.0171","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Directed flow of charged particles is studied in
nucleus-nucleus collisions simulated within the energy range accessible
for NICA and FAIR facilities. Two transport cascade models, UrQMD and
QGSM, are employed. These models use different mechanisms of the string
excitation and string fragmentation. Despite of the differences,
directed flows of charged pions and charged kaons in both models remain
antiflow-oriented with reduction of the collision energy from $\sqrt{s}
= 11.5$~GeV to 3.5~GeV. In contrast, the directed flow of protons
changes its sign from antiflow to normal flow within the investigated
energy interval. Both models favor continuous non-uniform emittence of
hadrons from the expanding fireball rather than sharp, or sudden,
freeze-out picture adopted by majority of hydrodynamic models. We found
that the earlier frozen hadrons carry the strongest directed flow at
midrapidity, although the flow development even at $|y| \leq 0.5$ takes
about 8-12~fm/$c$ for different hadron species.