1994
DOI: 10.1016/0375-9474(94)90923-7
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Relativistic mean-field theory for unstable nuclei with non-linear σ and ω terms

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Cited by 983 publications
(1,129 citation statements)
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References 14 publications
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“…Here we find that sets IV and V match with NL3 and DBHF, respectively up to three times the nuclear matter density. It is to be noted that the EOS obtained by DBHF is trusted upto two times of nuclear matter density [36,37]. The difference between the two sets IV (stiff) and V (soft) is only due to the different effective mass for the same incompressibility (K = 300 MeV).…”
Section: At Zero Temperature Limitmentioning
confidence: 90%
“…Here we find that sets IV and V match with NL3 and DBHF, respectively up to three times the nuclear matter density. It is to be noted that the EOS obtained by DBHF is trusted upto two times of nuclear matter density [36,37]. The difference between the two sets IV (stiff) and V (soft) is only due to the different effective mass for the same incompressibility (K = 300 MeV).…”
Section: At Zero Temperature Limitmentioning
confidence: 90%
“…For the treatment of nuclear interactions, we employ the relativistic mean-field (RMF) model with the TM1 parameter set [21], where nucleons interact via the exchange of isoscalar scalar and vector mesons (σ and ω) and isovector vector meson (ρ). The nucleonic Lagrangian density reads…”
Section: Relativistic Mean-field Model and Thomas-fermi Approximationmentioning
confidence: 99%
“…From the Lagrangian density (1), we derive the equations of motion for nucleons and meson mean fields, which can be solved self-consistently. The TM1 parametrization of the RMF model was found to be successful in describing the ground-state properties of finite nuclei and infinite nuclear matter [21]. In order to examine the influence of the symmetry energy slope L, we use a set of generated models based on the TM1 parametrization as described in our previous work [22].…”
Section: Relativistic Mean-field Model and Thomas-fermi Approximationmentioning
confidence: 99%
“…Again the interaction between a pair of nucleons when they are embedded in a heavy nucleus is less than the force in empty space. This suppression of the two-body interactions within a nucleus in favour of the interaction of each nucleon with the average nucleon density, means that the non-linearity acts as a smoothing mechanism and hence leads in the direction of the one-body potential and shell structure 17,18,19,20 . The replacement of mass term 1 2 m 2 σ σ 2 of σ field by U (σ) and 1 2 m 2 ω V µ V µ of ω field by U (ω).…”
Section: Non-linear Casementioning
confidence: 99%