2016
DOI: 10.1103/physrevc.94.044622
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Thermal and transport properties in central heavy-ion reactions around a few hundred MeV/nucleon

Abstract: Thermalization process of nuclear matter in central fireball region of heavy-ion collisions is investigated by employing an extension model of Boltzmann-Uehling-Uhlenbeck, namely the Van der Waals Boltzmann-Uehling-Uhlenbeck (VdWBUU) model. Temperature (T ) is extracted by the quantum Fermion fluctuation approach and other thermodynamic quantities, such as density (ρ), entropy density (s), shear viscosity (η), isospin diffusivity (DI ) and heat conductivity (κ), are also deduced. The liquid-like and gas-like p… Show more

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Cited by 18 publications
(16 citation statements)
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“…The minimum in this picture is related to the breakdown of the hydrodynamics expansion [30]. A minimum for η/s was also discussed in holographic models where it corresponds to a transition between thermal gas background and a big black hole solution at high temperature [31], and in certain nuclear matter models [32,33].…”
Section: Kinematic Viscositymentioning
confidence: 98%
“…The minimum in this picture is related to the breakdown of the hydrodynamics expansion [30]. A minimum for η/s was also discussed in holographic models where it corresponds to a transition between thermal gas background and a big black hole solution at high temperature [31], and in certain nuclear matter models [32,33].…”
Section: Kinematic Viscositymentioning
confidence: 98%
“…The minimum in this picture is related to the breakdown of the hydrodynamics expansion [29]. A minimum for η/s was also discussed in holographic models where it corresponds to a transition between thermal gas background and a big black hole solution at high temperature [30], and in certain nuclear matter models [31,32].…”
Section: Kinematic Viscositymentioning
confidence: 98%
“…At zero temperature, the properties of nuclear matter have been studied extensively, and its equation of state (EOS), including its isospin dependence, i.e., symmetry energy, has been determined relatively well [1][2][3], while its properties at finite temperature are relatively little touched upon. Among these properties, two noticeable examples are the nuclear liquid-gas phase transition [4][5][6][7][8][9][10][11][12][13][14][15][16] and the temperature dependence of the ratio of shear viscosity to entropy density (η/s) [17][18][19][20][21][22]. The latter is also connected to the nuclear giant dipole resonance at finite temperature [23][24][25], since both of them are related to the two-body dissipation of nucleons.…”
Section: Introductionmentioning
confidence: 99%