2010
DOI: 10.1140/epja/i2010-10983-1
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A relativistic approach to the equation of state of asymmetric nuclear matter

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Cited by 22 publications
(7 citation statements)
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“…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]. The LOCV calculation is a fully self-consistent technique with state-dependent correlation functions.…”
Section: The Variational Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…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]. The LOCV calculation is a fully self-consistent technique with state-dependent correlation functions.…”
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%
“…Later on, this approach was extended to finite temperature [47] and also calculations of the EoS of asymmetric nuclear matter [48], pure neutron matter, and β-stable matter [49,50] were carried out within this framework by using more sophisticated potentials. Moreover, relativistic corrections have been considered in calculating thermodynamic properties of nuclear matter within this model at both zero and finite temperatures [51,52]. Recently, this technique has been extended by adding TBF to this formalism [53,54], and has been used to study the structure of the NS [53] as well as proto-neutron star [54].…”
Section: Introductionmentioning
confidence: 99%
“…The reason is that the EOS of hadron matter governs the star in the hadron branch and as is clear from Eqs. ( 31), ( 32) and (33), y R , which depends on the profile of the star, takes the same value, so k 2 and hence Λ, from Eqs ( 30) and ( 29) will have a unique value for the same hadron interaction. In these cases, the HSs become much less compact, and tidal defromability takes larger values in comparison with the cases in which the mass of 1.4M ⊙ occur on the quark branch.…”
Section: Tidal Deformabilitymentioning
confidence: 99%
“…This approach is extended in such a way to enable one to calculate the properties of asymmetric nuclear matter, neutron matter and beta stable matter EOSs at both zero and finite temperatures by using more sophisticated potentials [29][30][31][32]. Besides this, the thermodynamic properties of nuclear matter at both zero and finite temperatures are calculated by considering relativistic corrections in this formalism [33,34]. It is well known that the bare two-body nucleonnucleon (2BF) interactions cannot reproduce the saturation properties of nuclear matter.…”
Section: Introductionmentioning
confidence: 99%