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By L. Beaulieu, T. Lefort, W. C-Hsi, K. Kwiatkowski (auth.), Wolfgang Bauer, Gary D. Westfall (eds.)

th This workshop used to be the 15 in a sequence that addresses the topic of the dynamics of nuclear reactions. those workshops are devoted to the concept bringing jointly scientists from various components of nuclear reactions promotes the colourful trade of principles. This workshop hosted displays from experimentalists and theorists, intermediate strength to ultrarelativistic energies, and outcome to fresh speculations. a lot of those scientists wouldn't ordinarily be uncovered to the paintings performed in different subfields. hence the iciness Workshop on Nuclear Dynamics performs a different function in info alternate and the stimulation of recent ides. the sphere of nuclear dynamics has a vibrant destiny. New accelerators are being deliberate and accomplished worldwide. New detectors are being developed. New types and theories are being built to explain those phenomena. The iciness Workshop on Nuclear Dynamics will proceed to advertise this full of life and compelling box of analysis. WOLFGANG BAUER AND GARY D. WESTFALL v earlier Workshops the next desk incorporates a checklist of the dates and destinations of the former iciness Workshops on Nuclear Dynamics in addition to the contributors of the organizing committees. The chairpersons of the meetings are underlined.

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Wiedemann, private communication. [17] F. Becattini, M. Gazdzicki, and J. Sollfrank, Eur. Phys. J. C 5 (1998) 143. R. Nix, Phys. Rev. C 58 (1998) 2303. Chapter 4 HADRON FREEZE-OUT AND QGP HADRONIZATION J. Rafelski and J. Letessier Department of Physics, University of Arizona, Tucson, AZ 85721, USA* Laboratoire de Physique Theorique et Hautes Energies t Universite Paris 7, 2 place Jussieu, F-75251 Cedex 05. S. Department of Energy, DE-FG03-95ER40937. tLPTHE, Univ. Paris 6 et 7 is: Unite mixte de Recherche du CNRS, UMR 7589.

We also vary "fa, keeping "fq = 1. A nearly valid experimental data description is now possible, and indeed, when the error bars were smaller this was a satisfactory approach adapted in many studies [1]. However, only the possibility of light quark non-equilibrium in fit D produces a statistically significant data description. It is interesting to note that a significant degradation of occurs, especially in the Pb-Pb data, when we require in column F that the particle ratios comprising a and a-particles are also described.

2 GeV per participating nucleon. Considerable refinement of data analysis has occurred since last comprehensive review of the field [1]. Our present work includes in particular the following: 1. We considered aside of strange also light quark (q = u, d) chemical non-equilibrium abundance [2] and introduce along with the statistical strangeness non-equilibrium parameter {S, its light quark analogue {q' 2. Coulomb distortion of the strange quark phase space has been understood [3]. Incorporating these developments, we accurately describe abundances of strange as well as non-strange hadrons, both at central rapidity and in 41l'-acceptance.

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