2007
DOI: 10.1016/j.nuclphysa.2007.04.013
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Thermal properties of asymmetrical nuclear matter with the new charge-dependent Reid potential

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Cited by 31 publications
(14 citation statements)
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“…This method was reformulated to include more sophisticated interactions [34], such as UV 14 , AV 18 [35], and charge-dependent Reid potential (Reid93) [36]. The LOCV method has been also developed for calculating the various thermodynamic properties of hot and frozen homogeneous fermionic fluids, such as symmetric and asymmetric nuclear matter [37], β-stable matter [38], helium-3 [39], and electron fluid [40], with different realistic interactions. Recently, the LOCV formalism was developed for covering the relativistic Hamiltonian with a potential that has been fitted relativistically to nucleon-nucleon phase shifts [41].…”
Section: The Variational Methodsmentioning
confidence: 99%
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“…This method was reformulated to include more sophisticated interactions [34], such as UV 14 , AV 18 [35], and charge-dependent Reid potential (Reid93) [36]. The LOCV method has been also developed for calculating the various thermodynamic properties of hot and frozen homogeneous fermionic fluids, such as symmetric and asymmetric nuclear matter [37], β-stable matter [38], helium-3 [39], and electron fluid [40], with different realistic interactions. Recently, the LOCV formalism was developed for covering the relativistic Hamiltonian with a potential that has been fitted relativistically to nucleon-nucleon phase shifts [41].…”
Section: The Variational Methodsmentioning
confidence: 99%
“…In this equation, V (1, 2) is a phenomenological nucleon-nucleon potential such as Reid type, UV 14 , and AV 18 . At this stage, we can minimize the twobody energy with respect to the variations of the correlation functions [33,34,36] but subject to the normalization constraint [33][34][35][36][37][38][39][40][41]:…”
Section: The Variational Methodsmentioning
confidence: 99%
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“…Although significant efforts have been devoted to the study of the properties of cold asymmetric nuclear matter during the last decade, much less attention has so far been paid to those of hot asymmetric nuclear matter, especially the temperature dependence of the nuclear symmetry energy [212,213,[339][340][341][342][343]. For finite nuclei at temperatures below about 3 MeV, the shell structure and pairing effects as well as vibrations of nuclear surfaces remain important, and the symmetry energy was predicted to increase only slightly with increasing temperature [344][345][346].…”
Section: Temperature Dependence Of the Symmetry Energy And The Thermamentioning
confidence: 99%
“…As in the case of zero temperature, studies based on both phenomenological and microscopic models [212,339,340,342,343,364] have indicated that the EOS of hot asymmetric nuclear matter at density ρ, temperature T , and an isospin asymmetry δ can also be written as a parabolic function of δ, i.e.,…”
Section: Nuclear Symmetry Energy At Finite Temperaturementioning
confidence: 99%