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From our previously obtained shear viscosity to entropy density ratio ($eta/s$) in the framework of clustering of color sources (Color String Percolation Model: CSPM), we calculate the jet quenching parameter $hat {q}$ and trace anomaly $Delta = (varepsilon -3it p)/T^{4}$ as a function of temperature. It is shown that the scaled $hat {q}/T^{3}$ is in agreement with the recent JET Collaboration estimates. The inverse of $eta/s$ is found to represent $Delta$. The results for $Delta$ are in excellent agreement with Lattice Quantum Chromo Dynamics (LQCD) simulations. From the trace anomaly and energy density $epsilon$, the equation of state is obtained as a function of temperature and compared with LQCD simulations. It is possible that there is a direct connection between the $eta/s$ and $Delta$. Thus the estimate of transport coefficient $eta/s$ provides $hat {q}$ and $Delta$ as a function of temperature. Both $Delta$ and $eta/s$ describe the transition from a strongly coupled QGP to a weakly coupled QGP.
A thermodynamic quantum many-body $T$-matrix approach is employed to study the spectral and transport properties of the quark-gluon plasma at moderate temperatures where nonperturbative effects are essential. For the partonic two-body interaction we
A brief introduction of the relationship of string percolation to the Quantum Chromo Dynamics (QCD) phase diagram is presented. The behavior of the Polyakov loop close to the critical temperature is studied in terms of the color fields inside the clu
We consider the most general fractional background fluxes in the color, flavor, and baryon number directions, compatible with the faithful action of the global symmetry of a given theory. We call the obstruction to gauging symmetries revealed by such
We present lattice calculations of the low-lying spectrum of $^{12}$C using a simple nucleon-nucleon interaction that is independent of spin and isospin and therefore invariant under Wigners SU(4) symmetry. We find strong signals for all excited stat
Possible phase transition of strongly interacting matter from hadron to a quark-gluon plasma state have in the past received c onsiderable interest. It has been suggested that this problem might be treated by percolation theory. The clustering of col