Directed Flow in Heavy-Ion Collisions and Its Implications for Astrophysics

Analysis of directed flow ( v 1 ) of protons, antiprotons and pions in heavy-ion collisions is performed in the range of collision energies s N N = 2.7–39 GeV. Simulations have been done within a three-fluid model employing a purely hadronic equation of state (EoS) and two versions...

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Main Author: Yuri B. Ivanov
Format: Article
Language:English
Published: MDPI AG 2017-11-01
Series:Universe
Subjects:
Online Access:https://www.mdpi.com/2218-1997/3/4/79
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author Yuri B. Ivanov
author_facet Yuri B. Ivanov
author_sort Yuri B. Ivanov
collection DOAJ
description Analysis of directed flow ( v 1 ) of protons, antiprotons and pions in heavy-ion collisions is performed in the range of collision energies s N N = 2.7–39 GeV. Simulations have been done within a three-fluid model employing a purely hadronic equation of state (EoS) and two versions of the EoS with deconfinement transitions: a first-order phase transition and a smooth crossover transition. The crossover EoS is unambiguously preferable for the description of experimental data at lower collision energies s N N ≲ 20 Gev. However, at higher collision energies s N N ≳ 20 Gev. the purely hadronic EoS again becomes advantageous. This indicates that the deconfinement EoS in the quark-gluon sector should be stiffer at high baryon densities than those used in the calculation. The latter finding is in agreement with that discussed in astrophysics in connection with existence of hybrid stars with masses up to about two solar masses.
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spelling doaj.art-053c389fc00247c993a00976505c3e7c2022-12-22T04:01:40ZengMDPI AGUniverse2218-19972017-11-01347910.3390/universe3040079universe3040079Directed Flow in Heavy-Ion Collisions and Its Implications for AstrophysicsYuri B. Ivanov0National Research Centre (NRC) “Kurchatov Institute”, Moscow 123182, RussiaAnalysis of directed flow ( v 1 ) of protons, antiprotons and pions in heavy-ion collisions is performed in the range of collision energies s N N = 2.7–39 GeV. Simulations have been done within a three-fluid model employing a purely hadronic equation of state (EoS) and two versions of the EoS with deconfinement transitions: a first-order phase transition and a smooth crossover transition. The crossover EoS is unambiguously preferable for the description of experimental data at lower collision energies s N N ≲ 20 Gev. However, at higher collision energies s N N ≳ 20 Gev. the purely hadronic EoS again becomes advantageous. This indicates that the deconfinement EoS in the quark-gluon sector should be stiffer at high baryon densities than those used in the calculation. The latter finding is in agreement with that discussed in astrophysics in connection with existence of hybrid stars with masses up to about two solar masses.https://www.mdpi.com/2218-1997/3/4/79heavy-ion collisionsdirected flowhydrodynamicsdeconfinementhybrid stars
spellingShingle Yuri B. Ivanov
Directed Flow in Heavy-Ion Collisions and Its Implications for Astrophysics
Universe
heavy-ion collisions
directed flow
hydrodynamics
deconfinement
hybrid stars
title Directed Flow in Heavy-Ion Collisions and Its Implications for Astrophysics
title_full Directed Flow in Heavy-Ion Collisions and Its Implications for Astrophysics
title_fullStr Directed Flow in Heavy-Ion Collisions and Its Implications for Astrophysics
title_full_unstemmed Directed Flow in Heavy-Ion Collisions and Its Implications for Astrophysics
title_short Directed Flow in Heavy-Ion Collisions and Its Implications for Astrophysics
title_sort directed flow in heavy ion collisions and its implications for astrophysics
topic heavy-ion collisions
directed flow
hydrodynamics
deconfinement
hybrid stars
url https://www.mdpi.com/2218-1997/3/4/79
work_keys_str_mv AT yuribivanov directedflowinheavyioncollisionsanditsimplicationsforastrophysics