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      Isospin effect in the statistical sequential decay

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          Abstract

          Isospin effect of the statistical emission fragments from the equilibrated source is investigated in the frame of statistical binary decay implemented into GEMINI code, isoscaling behavior is observed and the dependences of isoscaling parameters \(\alpha\) and \(\beta\) on emission fragment size, source size, source isospin asymmetry and excitation energies are studied. Results show that \(\alpha\) and \(\beta\) neither depends on light fragment size nor on source size. A good linear dependence of \(\alpha\) and \(\beta\) on the inverse of temperature \(T\) is manifested and the relationship of \(\alpha=4C_{sym}[(Z_{s}/A_{s})_{1}^{2}-(Z_{s}/A_{s})_{2}^{2}]/T\) and \(\beta=4C_{sym}[(N_{s}/A_{s})_{1}^{2}-(N_{s}/A_{s})_{2}^{2}]/T\) from different isospin asymmetry sources are satisfied. The symmetry energy coefficient \(C_{sym}\) extracted from simulation results is \(\sim\) 23 MeV which includes both the volume and surface term contributions, of which the surface effect seems to play a significant role in the symmetry energy.

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          Unified nuclear potential for heavy-ion elastic scattering, fusion, fission, and ground-state masses and deformations

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            Isospin Physics in Heavy-Ion Collisions at Intermediate Energies

            In nuclear collisions induced by stable or radioactive neutron-rich nuclei a transient state of nuclear matter with an appreciable isospin asymmetry as well as thermal and compressional excitation can be created. This offers the possibility to study the properties of nuclear matter in the region between symmetric nuclear matter and pure neutron matter. In this review, we discuss recent theoretical studies of the equation of state of isospin-asymmetric nuclear matter and its relations to the properties of neutron stars and radioactive nuclei. Chemical and mechanical instabilities as well as the liquid-gas phase transition in asymmetric nuclear matter are investigated. The in-medium nucleon-nucleon cross sections at different isospin states are reviewed as they affect significantly the dynamics of heavy ion collisions induced by radioactive beams. We then discuss an isospin-dependent transport model, which includes different mean-field potentials and cross sections for the proton and neutron, and its application to these reactions. Furthermore, we review the comparisons between theoretical predictions and available experimental data. In particular, we discuss the study of nuclear stopping in terms of isospin equilibration, the dependence of nuclear collective flow and balance energy on the isospin-dependent nuclear equation of state and cross sections, the isospin dependence of total nuclear reaction cross sections, and the role of isospin in preequilibrium nucleon emissions and subthreshold pion production.
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              Isotopic Scaling in Nuclear Reactions

              A three parameter scaling relationship between isotopic distributions for elements with Z\(\leq 8\) has been observed that allows a simple description of the dependence of such distributions on the overall isospin of the system. This scaling law (termed iso-scaling) applies for a variety of reaction mechanisms that are dominated by phase space, including evaporation, multifragmentation and deeply inelastic scattering. The origins of this scaling behavior for the various reaction mechanisms are explained. For multifragmentation processes, the systematics is influenced by the density dependence of the asymmetry term of the equation of state.
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                Author and article information

                Journal
                15 February 2007
                2007-07-27
                Article
                10.1103/PhysRevC.76.024607
                nucl-th/0702052
                76a3a8f8-ed85-4400-81d0-0549ee4386be
                History
                Custom metadata
                Phys.Rev.C76:024607,2007
                8 pages, 8 figures; A new substantially modified version which has been accepted by the Physical Review C
                nucl-th math-ph math.MP nucl-ex

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