1. Cosmological QCD phase transition in steady non-equilibrium dissipative Hořava–Lifshitz early universe
- Author
-
M. Khodadi and H. R. Sepangi
- Subjects
High Energy Physics - Theory ,Physics ,Quantum chromodynamics ,Phase transition ,Deceleration parameter ,media_common.quotation_subject ,General Physics and Astronomy ,Volume viscosity ,General Relativity and Quantum Cosmology ,Cosmology ,Universe ,Physics::Fluid Dynamics ,Chiral symmetry breaking ,Scale factor (cosmology) ,Mathematical physics ,media_common - Abstract
We study the phase transition from quark-gluon plasma to hadrons in the early universe in the context of non-equilibrium thermodynamics. According to the standard model of cosmology, a phase transition associated with chiral symmetry breaking after the electro-weak transition has occurred when the universe was about $1-10\mu s$ old. We focus attention on such a phase transition in the presence of a viscous relativistic cosmological background fluid in the framework of non-detailed balance Ho\v{r}ava-Lifshitz cosmology within an effective model of QCD. We consider a flat Friedmann-Robertson-Walker Universe filled with a non-causal and causal bulk viscous cosmological fluid respectively and investigate the effects of the running coupling constants of Ho\v{r}ava-Lifshitz gravity, $\lambda$, on the evolution of the physical quantities relevant to a description of the early universe, namely, the temperature $T$, scale factor $a$, deceleration parameter $q$ and dimensionless ratio of the bulk viscosity coefficient to entropy density $\frac{\xi}{s}$. We assume that the bulk viscosity cosmological background fluid obeys the evolution equation of the steady truncated (Eckart) and full version of the Israel-Stewart fluid, respectively., Comment: 21 pages, 16 figures
- Published
- 2014