2002
DOI: 10.1016/s0375-9474(02)01018-7
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High density behaviour of nuclear symmetry energy and high energy heavy-ion collisions

Abstract: High energy heavy-ion collisions are proposed as a novel means to constrain stringently the high density (HD) behaviour of nuclear symmetry energy. Within an isospin-dependent hadronic transport model, it is shown for the first time that the isospin asymmetry of the HD nuclear matter formed in high energy heavyion collisions is uniquely determined by the HD behaviour of nuclear symmetry energy. Experimental signatures in two sensitive probes, i.e., π − to π + ratio and neutron-proton differential collective fl… Show more

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Cited by 132 publications
(64 citation statements)
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“…The symmetry energy is found to affect several aspects of high energy heavy-ion collisions; in particular, the neutron/proton ratio of high density nuclear matter is expected to be determined mainly by the high density behavior of a 4 [38]. The current self-consistent approximation shows that a 4 is strongly correlated to the effective mass of ρ-meson, m * ρ .…”
Section: Symmetry Energymentioning
confidence: 99%
“…The symmetry energy is found to affect several aspects of high energy heavy-ion collisions; in particular, the neutron/proton ratio of high density nuclear matter is expected to be determined mainly by the high density behavior of a 4 [38]. The current self-consistent approximation shows that a 4 is strongly correlated to the effective mass of ρ-meson, m * ρ .…”
Section: Symmetry Energymentioning
confidence: 99%
“…Calculations predict that central densities of two to three times the saturation density may be reached in 197 Au+ 197 Au collisions at 400 to 1000 MeV/nucleon on time scales of ≈ 10 − 20 fm/c [87]. The resulting pres-sure produces a collective outward motion of the compressed material whose strength, differentiating between neutrons and protons, is influenced by the symmetry energy in asymmetric systems [25].…”
Section: Density Probedmentioning
confidence: 99%
“…As to the mean-field potential of ∆ resonances in nuclear medium [14,19], it is commonly assumed in transport models that its isoscalar part is the same as that for nucleon, but its isovector part is taken to be the weighted average of those for neutron and proton according to the squared Clebsch-Gordan coefficients from * zhenzhang@comp.tamu.edu † ko@comp.tamu.edu its isospin structure [1,20]. This assumption leads to a change between the initial and final potentials in some of the processes N + N ↔ N + ∆ and ∆ ↔ N + π.…”
Section: Introductionmentioning
confidence: 99%