A phenomenological test of the independent quasi-particle model

1967 ◽  
Vol 103 (2) ◽  
pp. 257-299 ◽  
Author(s):  
Vincent Gillet ◽  
Bertrand Giraud ◽  
Mannque Rho
Author(s):  
Ameng Zhao ◽  
Xiaofeng Luo ◽  
Hongshi Zong

2020 ◽  
Vol 12 (2) ◽  
pp. 215-221
Author(s):  
P. K. Sethy ◽  
Y. Kumar ◽  
S. S. Singh

It is believed that a transient strong magnetic field is generated in heavy-ion collision. The strength of this field perpendicular to the reaction plane and is estimated to be around eB=0.03GeV2 at RHIC and eB=0.3GeV2 at LHC. We study the effect of this magnetic field on dilepton yield using a modified quasi particle model. The results show a clear enhancement in dilepton yield and our result is in good agreement with the recently reported results.


2014 ◽  
Vol 29 (10) ◽  
pp. 1450056 ◽  
Author(s):  
Vishnu M. Bannur

Landau's formalism of statistical mechanics [following L. D. Landau and E. M. Lifshitz, Statistical Physics (Pergamon Press, Oxford, 1980)] is applied to the quasi-particle model of quark–gluon plasma. Here, one starts from the expression for pressure and develop all thermodynamics. It is a general formalism and consistent with our earlier studies [V. M. Bannur, Phys. Lett. B647, 271 (2007)] based on Pathria's formalism [following R. K. Pathria, Statistical Mechanics (Butterworth-Heinemann, Oxford, 1977)]. In Pathria's formalism, one starts from the expression for energy density and develop thermodynamics. Both the formalisms are consistent with thermodynamics and statistical mechanics. Under certain conditions, which are wrongly called thermodynamic consistent relation, we recover other formalism of quasi-particle system, like in M. I. Gorenstein and S. N. Yang, Phys. Rev. D52, 5206 (1995), widely studied in quark–gluon plasma.


2016 ◽  
Vol 763 ◽  
pp. 139-144 ◽  
Author(s):  
E.P. Politis ◽  
C.E. Tsagkarakis ◽  
F.K. Diakonos ◽  
X.N. Maintas ◽  
A. Tsapalis

2012 ◽  
Vol 29 (10) ◽  
pp. 101201 ◽  
Author(s):  
Yan Yan ◽  
Jing Cao ◽  
Xin-Lian Luo ◽  
Wei-Min Sun ◽  
Hong-Shi Zong

2006 ◽  
Vol 27 (4) ◽  
pp. 397-402 ◽  
Author(s):  
M. Bluhm ◽  
B. Kämpfer ◽  
R. Schulze ◽  
D. Seipt

2010 ◽  
Vol 848 (3-4) ◽  
pp. 330-340 ◽  
Author(s):  
Vinod Chandra ◽  
V. Ravishankar

2019 ◽  
Vol 2019 ◽  
pp. 1-13
Author(s):  
Indrani Nilima ◽  
Vineet Kumar Agotiya

The present article is the follow-up of our work Bottomonium suppression in quasi-particle model, where we have extended the study for charmonium states using quasi-particle model in terms of quasi-gluons and quasi quarks/antiquarks as an equation of state. By employing medium modification to a heavy quark potential thermodynamic observables, viz., pressure, energy density, speed of sound, etc. have been calculated which nicely fit with the lattice equation of state for gluon, massless, and as well massive flavored plasma. For obtaining the thermodynamic observables we employed the debye mass in the quasi particle picture. We extended the quasi-particle model to calculate charmonium suppression in an expanding, dissipative strongly interacting QGP medium (SIQGP). We obtained the suppression pattern for charmonium states with respect to the number of participants at mid-rapidity and compared it with the experimental data (CMS JHEP) and (CMS PAS) at LHC energy (Pb+Pb collisions, sNN = 2.76 TeV).


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