Abstract
The color confinement in Quantum Chromodynamics (QCD) remains an interesting and intriguing phenomenon. It is considered as a very important nonperturbative effect to be taken into account in all models intended to describe the QCD many-parton system. During the deconfinement phase transition, the non-Abelian character of the partonic plasma manifests itself in an important manner. A direct consequence of color confinement is that all states of any partonic system must be colorless and the requirement of the colorlessness condition is more than necessary. Indeed, the colorless state is a result of the multiparton interactions, from which collective phenomena can emerge, inducing strong correlations and giving rise to a long-range order of liquid-like phase, a behavior fundamentally different from that of a conformal ideal gas. Within our Colorless QCD MIT-Bag Model and using the [Formula: see text]-method, three Thermal Response Functions, related to the Equation of State, like pressure [Formula: see text], sound velocity [Formula: see text] and energy density [Formula: see text] are calculated and studied as functions of temperature [Formula: see text] and volume [Formula: see text]. Also and in the same context, two relevant correlation forms [Formula: see text] and [Formula: see text] are calculated and studied intensively as functions of [Formula: see text] at different volumes. A detailed comparative study between our results and those obtained from lattice QCD simulation, hot QCD and other phenomenological models is carried out. We find that the Liquid Partonic Plasma Model is the model which fits our Equation of State very well, in which the Bag constant term is revealed very important. Our Colorless Partonic Plasma, just beyond the finite volume transition point, is found in a state where the different partons interact strongly showing a liquid behavior in agreement with the estimate of the plasma parameter [Formula: see text] and supporting the result obtained from the fitting work. This allows us to understand experimental observations in Ultra-Relativistic Heavy-Ion Collisions and to interpret lattice QCD results.
Highlights
The Quantum Chromodynamics (QCD) Equation of State (EoS) is of crucial importance for a better comprehension of the strongly interacting matter created in the Ultra-Relativistic Heavy-Ion Collisions (URHIC).[4]
The confinement phenomenon concerns any many-parton system, and the colorlessness condition can be considered as an effect of the color interaction between partons rendering the system to be in a colorless state
In the phenomenological approaches of URHIC physics, we always need an EoS to model the hydrodynamic expansion of the system
Summary
The Quantum Chromodynamics (QCD) Equation of State (EoS) is of crucial importance for a better comprehension of the strongly interacting matter created in the Ultra-Relativistic Heavy-Ion Collisions (URHIC).[4]. That in order to understand the physical properties at finite temperature of strongly interacting matter the study of its EoS is of great importance It highlights the intimate relationship between the degrees of freedom and the different phases of the system. The system exhibits, by definition, a singular behavior in some Thermal Response Function (TRF), which appears only in the thermodynamic limit.[5] In both experimental and lattice QCD investigations, we are dealing with finite volume systems They require the development of theoretical approaches that can be able to accurately describe the phase transition in finite-volume including the colorlessness condition. Such an effect has been found,[10] relating the multiparticle production to the finite volume of the reaction region in an URHIC
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