Abstract
A major goal in the study of relativistic heavy ion collisions is to measure the nuclear equation of state (EOS). The interpretation of the experimental data such as the transverse flow are based on simulations of the Boltzmann equation, which combine the nuclear mean field and individual nucleon-nucleon collisions as dynamical input. It has been found that most observables are affected by both ingredients1,2.
Work supported by BMFT and GSI Darmstadt.
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References
G. F. Bertsch , Nucl.Phys.A490 745 (1988)
G. F. Bertsch , Phys.Lett.189B 384 (1987)
B ter Haar and R. Malfliet, Phys.Repts.149 207 (1987)
F. de Jong and R. Malfliet, these proceedings
C. Gale , Phys.Rev.C35 1666 (1987) J. Aichelin , Phys.Rev.Lett.59 1926 (1987) B. Blättel , Phys.Rev.C38 1767 (1988)
G. M. Welke , Phys.Rev.C38 2101 (1988)
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© 1989 Plenum Press, New York
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Koch, V. (1989). Momentum Dependent Potentials in Relativistic Heavy Ion Collisions. In: Soyeur, M., Flocard, H., Tamain, B., Porneuf, M. (eds) Nuclear Matter and Heavy Ion Collisions. NATO ASI Series, vol 205. Springer, Boston, MA. https://doi.org/10.1007/978-1-4684-5715-5_26
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DOI: https://doi.org/10.1007/978-1-4684-5715-5_26
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