2005
DOI: 10.1016/j.nuclphysa.2004.12.018
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The limiting Temperature of hot nuclei from microscopic Equation of State

Abstract: The limiting temperature T lim of a series of nuclei is calculated employing a set of microscopic nuclear Equations of State (EoS). It is shown that the value of T lim is sensitive to the nuclear matter Equation of State used. Comparison with the values extracted in recent phenomenological analysis appears to favour a definite selection of EoS' s. On the basis of this phenomenological analysis, it seems therefore possible to check the microscopic calculations of the nuclear EoS at finite temperature, which is … Show more

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Cited by 3 publications
(2 citation statements)
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“…The nucleus, which resembles a hot liquid drop, expands because of thermal pressure and moves to the spinodal region where it is surrounded by a nucleon gas. As the spinodal is the region of instability, the nucleus explodes violently and the process is known as multi-fragmentation at freeze-out volume ≈ 7V 0 [13] There have been several qualitative attempts to study the limiting temperature of nuclei in terms of Coulomb instability, where the EoS of infinite matter is taken from various theoretical frameworks such as Skyrme effective NN interaction [14,15], microscopic EoS such as Friedman and Pandharipande, finite temperature relativistic Dirac-Brueckner, chiral perturbation theory [16][17][18], EoS considering the degeneracy of the Fermi system [19] relativistic calculations using quantum hadrodynamics and Thomas-Fermi approach [20][21][22], Gogny interactions [23], chiral symmetry model [24]. Some calculations have been carried out by analyzing the plateau in caloric curve obtained from various experimental observations [25].…”
Section: Introductionmentioning
confidence: 99%
“…The nucleus, which resembles a hot liquid drop, expands because of thermal pressure and moves to the spinodal region where it is surrounded by a nucleon gas. As the spinodal is the region of instability, the nucleus explodes violently and the process is known as multi-fragmentation at freeze-out volume ≈ 7V 0 [13] There have been several qualitative attempts to study the limiting temperature of nuclei in terms of Coulomb instability, where the EoS of infinite matter is taken from various theoretical frameworks such as Skyrme effective NN interaction [14,15], microscopic EoS such as Friedman and Pandharipande, finite temperature relativistic Dirac-Brueckner, chiral perturbation theory [16][17][18], EoS considering the degeneracy of the Fermi system [19] relativistic calculations using quantum hadrodynamics and Thomas-Fermi approach [20][21][22], Gogny interactions [23], chiral symmetry model [24]. Some calculations have been carried out by analyzing the plateau in caloric curve obtained from various experimental observations [25].…”
Section: Introductionmentioning
confidence: 99%
“…Furthermore, the nature of phase transition is also altered due to strong Coulomb interaction. In this context some authors prefer to define limiting temperature (T l ) instead of the critical temperature for the hot nuclei [28,29]. This is the maximum temperature above which Coulomb effects (together with the decrease in surface tension) lead to thermal dissociation of nuclei.…”
Section: Introductionmentioning
confidence: 99%