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 chain that addresses the topic of the dynamics of nuclear reactions. those workshops are devoted to the concept bringing jointly scientists from diversified components of nuclear reactions promotes the colourful trade of principles. This workshop hosted shows from experimentalists and theorists, intermediate strength to ultrarelativistic energies, and outcome to contemporary speculations. a lot of those scientists wouldn't in most cases be uncovered to the paintings performed in different subfields. hence the iciness Workshop on Nuclear Dynamics performs a special position in details alternate and the stimulation of recent ides. the sector of nuclear dynamics has a vibrant destiny. New accelerators are being deliberate and accomplished all over the world. New detectors are being built. New types and theories are being constructed to explain those phenomena. The wintry weather Workshop on Nuclear Dynamics will proceed to advertise this energetic and compelling box of analysis. WOLFGANG BAUER AND GARY D. WESTFALL v prior Workshops the next desk incorporates a record 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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Extra info for Advances in Nuclear Dynamics 5
On the contrary, when comparing semi-peripheral Pb+Pb collisions with pp the exponent a varies over the entire PT interval, confirming the very different spectral shapes. N:t: 4. THERMAL FREEZEOUT A successful thermal interpretation of relativistic heavy ion collisions must provide an accurate description of the pion spectra since pions Particle Production in 158· A Ge V ... : ........ :.... :.. ~... Pltl. "........ ::......... -oo ... :......... T ........... 8 ....... ;......... :......... ; .........
S ! 5 . • . *~ .... • . r:::~;;:~~~~f1~~~:~:~~~F . ==~1;=T •Ni + Ni •• 0 . 5 . 4 but for the normalized neutral to charged pion ratio S~O). Experimental data (symbols) only exist for A + A reactions. the size Apart of the participant, but not in case of A + A reactions. The dependence on the excitation probability of the ~ resonance, listed in Fig. 2 by the percentages, is only weak. The comparison with the data shown by symbols indicates that to explain the p + A results one has to assume the presence of sufficiently many 7r N ~ loops, but that in the case of A + A reactions the number of such loops is much smaller since for both ratios one observes R~O) ~ S~O) ~ 1.
2] Metag, V. (1998) private communication. , et al. (1997) Z. Phys. A 359, 55. , et al. (1997) Z. Phys. A 357, 215.  Lemaire, M. , et al. (1988) Phys. Rev. c 43, 2711. , et al. (1997) Phys. Lett. B 407, 115. , et al. (1998) Eur. Phys. J. A 3,335.  Lisa, M. , et al. (1995) Phys. Rev. Lett. 75, 2662. , et al. (1998) Phys. Rev. C 57, 244. , et al. (1987) Phys. Rev. Lett. 58, 463. , et al. (1998) Eur. Phys. J. C 5, 129. , et al. (1991) Z. Phys. A 340, 325.  Hjort, E. , et al. (1997) Phys.
Advances in Nuclear Dynamics 5 by L. Beaulieu, T. Lefort, W. C-Hsi, K. Kwiatkowski (auth.), Wolfgang Bauer, Gary D. Westfall (eds.)