scholarly journals Towards the quark-gluon plasma Equation of State with dynamical strange and charm quarks

2016 ◽  
Vol 668 ◽  
pp. 012092 ◽  
Author(s):  
Florian Burger ◽  
Ernst-Michael Ilgenfritz ◽  
Maria Paola Lombardo ◽  
Michael Müller-Preussker ◽  
Anton Trunin
2002 ◽  
Vol 106-107 ◽  
pp. 528-530
Author(s):  
Peter N. Meisinger ◽  
Travis R. Miller ◽  
Michael C. Ogilvie

2012 ◽  
Vol 75 (7) ◽  
pp. 873-878 ◽  
Author(s):  
V. V. Begun ◽  
M. I. Gorenstein ◽  
O. A. Mogilevsky

2013 ◽  
Vol 04 (04) ◽  
pp. 13-20 ◽  
Author(s):  
Nabil M. El Naggar ◽  
Lotfy I. Abou-Salem ◽  
Ibrahim A. Elmashad ◽  
Ahmed Farag Ali

2011 ◽  
Vol 20 (08) ◽  
pp. 1805-1815 ◽  
Author(s):  
V. V. BEGUN ◽  
M. I. GORENSTEIN ◽  
O. A. MOGILEVSKY

The modified versions of the bag model equation of state (EoS) are considered. They are constructed to satisfy the main qualitative features observed for the quark–gluon plasma EoS in the lattice QCD calculations. A quantitative comparison with the lattice results at high temperatures T are done in the SU(3) gluodynamics and in the full QCD with dynamical quarks. Our analysis advocates a negative value of the bag constant B.


2007 ◽  
Vol 16 (07n08) ◽  
pp. 2048-2054 ◽  
Author(s):  
LI YAN ◽  
PENGFEI ZHUANG ◽  
NU XU

The charm quark thermalization in quark-gluon plasma is described by a transport model in relaxation time approximation. Combining the transport equation for charm quarks with the hydrodynamic description for the medium, we calculated the charm quark transverse momentum distribution and discussed its dependence on the relaxation time.


2020 ◽  
Vol 80 (7) ◽  
Author(s):  
Trambak Bhattacharyya ◽  
Abhik Mukherjee

Abstract We study the propagation of energy density perturbation in a hot, ideal quark–gluon medium in which quarks and gluons follow the Tsallis-like momentum distributions. We have observed that a non-extensive MIT bag equation of state obtained with the help of the quantum Tsallis-like distributions gives rise to a breaking wave solution of the equation dictating the evolution of energy density perturbation. However, the breaking of waves is delayed when the value of the Tsallis q parameter and the Tsallis temperature T are higher.


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