1988
DOI: 10.1103/physrevc.38.1003
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Nuclear equation of state from the nonlinear relativistic mean field theory

Abstract: The properties of symmetric nuclear matter are investigated in the nonlinear relativistic mean field theory of nuclear matter. We consider the constraints imposed by four nuclear ground state properties on the coupling constants and on the equation of state at Zero and at finite temperature. We find that the compression constant K(po) as well as the temperature is irrelevant for the stiffness of the equation of state for m 5 0.7. The main point is that the relativistic mean field theory exhibits acausal and un… Show more

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Cited by 70 publications
(58 citation statements)
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“…This allows a very good description of two important properties of nuclear matter, the compression modulus and the nucleon effective mass, which concerns the high-density behavior of the equation of state. However, some authors argue that the model suffers of a very serious problem: the constant c has negative values for several entries of M ⋆ and K, allowing the energy density to become unbounded from below for large values of the scalar meson mean field, leading to unphysical behaviour [18].…”
Section: Models With Derivative Couplingsmentioning
confidence: 99%
“…This allows a very good description of two important properties of nuclear matter, the compression modulus and the nucleon effective mass, which concerns the high-density behavior of the equation of state. However, some authors argue that the model suffers of a very serious problem: the constant c has negative values for several entries of M ⋆ and K, allowing the energy density to become unbounded from below for large values of the scalar meson mean field, leading to unphysical behaviour [18].…”
Section: Models With Derivative Couplingsmentioning
confidence: 99%
“…In addition it is well known from nuclear matter calculations [6][7][8][9][10][11] that in the temperature region under consideration (T < 20 MeV) nucleon-antinucleon pair production does not occur. Therefore we can neglect all antinucleon contributions.…”
Section: The Relativistic Thermal Thomas-fermi Approximation (Rttfa)mentioning
confidence: 99%
“…The densities of the two homogenous phases a and /3 are POt and P{3, respectively. To investigate the thermostatic properties of the finite system it is sufficient to look at the region ROt :5 r :5 R{3, since they are in principle known for the homogenous phases a (0 :5 r :5 ROt) and /3 (R{3 < r < 00) from nuclear matter calculations [6][7][8][9][10][11] (if there are no homogenous conditions in the bulk region of small nuclei, ROt = 0). In this region ROt < r < R{3 the transition between the "liquid" and the vapor phase takes place.…”
Section: Subtraction Mechanismmentioning
confidence: 99%
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“…Calculations done with lower effective masses show instabilities for highly dense nuclear systems such as 12c [26] and unphysical behavior in nuclear matter [27] for a negative coefficient C in the standard nonlinear selfinteraction of the effective scalar field [28,29]. Note that for a smaller effective mass one always gets a negative coefficient C (for a discussion of the parameter space and its shortcomings, see [30]).…”
Section: Single-a Hypernuclei In the Rmfmmentioning
confidence: 99%