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      Equation of State and Phase Transitions in the Nuclear and Hadronic Systems

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          Abstract

          An investigation of strongly interacting matter equation of state remains one of the major tasks of modern high energy nuclear physics for almost a quarter of century. The present work is my doctor of science thesis which contains my contribution (42 works) to this field made between 1993 and 2008. Inhere I mainly discuss the common physical and mathematical features of several exactly solvable statistical models which describe the nuclear liquid-gas phase transition and the deconfinement phase transition. Luckily, in some cases it was possible to rigorously extend the solutions found in thermodynamic limit to finite volumes and to formulate the finite volume analogs of phases directly from the grand canonical partition. It turns out that finite volume (surface) of a system generates also the temporal constraints, i.e. the finite formation/decay time of possible states in this finite system. Among other results I would like to mention the calculation of upper and lower bounds for the surface entropy of physical clusters within the Hills and Dales model; evaluation of the second virial coefficient which accounts for the Lorentz contraction of the hard core repulsing potential between hadrons; inclusion of large width of heavy quark-gluon bags into statistical description. I believe that the suggested mathematical solution of the freeze-out problem in relativistic hydrodynamic model and in hydro-cascade model has not only an academic interest, but also has some practical value. In addition I hope that the experience gained in working out some partly successful signals of deconfinement transition can be useful for other researchers to go further in this direction.

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          Structure of Matter below Nuclear Saturation Density

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            A Hydrodynamic Description of Heavy Ion Collisions at the SPS and RHIC

            A hydrodynamic + cascade model of relativistic heavy ion collisions is presented and compared to available hadronic data from the SPS to RHIC. The model consistently reproduces the radial and elliptic flow data for different particles, collision energies, and impact parameters. Three ingredients are essential to the success: (a) a reasonable EOS exhibiting the hard and soft features of the QCD phase transition, (b) thermal hadronization at the phase boundary, and (c) subsequent hadronic rescattering. Some features of the RHIC data are readily explained: (i) the observed elliptic flow and its dependence on \(p_{T}\) and mass, (ii) the anomalous \(\bar{p}/\pi^{-}\) ratio for \(p_{T} \approx 2.0\) GeV, (iii) the difference in the slope parameters measured by the STAR and PHENIX collaborations, and (iv) the respectively strong and weak impact parameter dependence of the \(\bar{p}\) and \(\phi\) slope parameters. For an EOS without the hard and soft features of the QCD phase transition, the broad consistency with the data is lost.
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              Radioactivity in strange quark matter

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                Author and article information

                Journal
                15 December 2010
                Article
                1012.3400
                490ea31c-1960-4671-8947-2dd76896171e

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
                Custom metadata
                Doctor of science thesis, 342 pages, 55 figures
                nucl-th

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