Abstract
The concepts of quark confinement and asymptotic freedom inherent in models of strongly interacting matter at the sub-hadronic level have lead to a great deal of interest in the associated deconfinement phase transition, i.e. the transition from a gas of Hadrons to a hot plasma of deconfined quarks and gluons. The possibility of obtaining energy densities which are large enough to cause deconfinement in ultra-relativistic heavy ion collisions has acted as one of the main stimuli to interest in such collisions, from both the experimental and theoretical points of view.
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Miller, H.G., Davidson, N.J., Quick, R.M., Plastino, A. (1992). Finite Size Effects in the Deconfinement Transition. In: Proto, A.N., Aliaga, J.L. (eds) Condensed Matter Theories. Condensed Matter Theories, vol 7. Springer, Boston, MA. https://doi.org/10.1007/978-1-4615-3352-8_35
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