2005
DOI: 10.1016/j.physrep.2004.12.004
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Reaction dynamics with exotic nuclei

Abstract: Iste magistrorum locus est simul et puerorum, mittunt quando volunt hic res quas perdere nolunt [1]. AbstractWe review the new possibilities offered by the reaction dynamics of asymmetric heavy ion collisions, using stable and unstable beams. We show that it represents a rather unique tool to probe regions of highly Asymmetric Nuclear Matter (AN M ) in compressed as well as dilute phases, and to test the in-medium isovector interaction for high momentum nucleons. The focus is on a detailed study of the symmetr… Show more

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Cited by 748 publications
(1,023 citation statements)
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References 220 publications
(279 reference statements)
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“…It can in principle vary from zero (in the case of a purely isoscalar phase separation), to infinity (in the case of a purely isovector instability, corresponding to a separation of protons from neutrons into two phases at the same baryon density). In practice δρ 3 /δρ is always a small number [5,20]. This is easy to understand considering that i) proton and neutron kinetic energies favour equal-size Fermi spheres and ii) the nuclear interaction is more attractive in the proton-neutron than the proton-proton and neutron-neutron channels in any realistic nuclear physics model (T = 0 contribution), which favours the existence of a mixed isospin bound phase.…”
Section: Direction Of Phase Separationmentioning
confidence: 99%
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“…It can in principle vary from zero (in the case of a purely isoscalar phase separation), to infinity (in the case of a purely isovector instability, corresponding to a separation of protons from neutrons into two phases at the same baryon density). In practice δρ 3 /δρ is always a small number [5,20]. This is easy to understand considering that i) proton and neutron kinetic energies favour equal-size Fermi spheres and ii) the nuclear interaction is more attractive in the proton-neutron than the proton-proton and neutron-neutron channels in any realistic nuclear physics model (T = 0 contribution), which favours the existence of a mixed isospin bound phase.…”
Section: Direction Of Phase Separationmentioning
confidence: 99%
“…Dynamical transport models [5,7] indicate that clusterization takes place at a relatively well-defined density inside the spinodal region determined by the collision dynamics and corresponding to the first development of instabilities, for which we take a typical value around ρ 0 /3. Spinodal decomposition is then a phenomenon fast enough for fragment formation dynamics to be dominated by the amplification of the most unstable modes at this density [10].…”
Section: Fractionation and Isocaling Observablesmentioning
confidence: 99%
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“…In laboratory experiments, this phase diagram can be explored only through heavy-ion collisions; in particular the multifragmentation phenomenon, observed for collisions around the Fermi energy and above, has been interpreted as the occurrence of the nuclear liquid-gas phase transition rounded by finite-size effects [4,5,6,7,8]. From the theoretical point of view, the isospin properties of the phase diagram have been studied extensively [9,10,11] and we know that the phase transition concerns isospin-symmetric (ρ n = ρ p ) as well as asymmetric (ρ n = ρ p ) matter.…”
Section: Introductionmentioning
confidence: 99%
“…In particular, the spinodal instabilities could be at the origin of the multifragmentation process [4,5,6]. Several models have been built in order to describe the dynamics leading to the formation of clusters [7,8]. Clustering is also expected to play an important role in compact stars [9,10].…”
Section: Introductionmentioning
confidence: 99%