scholarly journals Quartic isospin asymmetry energy of nuclear matter from chiral pion-nucleon dynamics

2015 ◽  
Vol 91 (6) ◽  
Author(s):  
N. Kaiser
1980 ◽  
Vol 92 (3-4) ◽  
pp. 261-264 ◽  
Author(s):  
E.Kh. Akhmedov ◽  
Yu.V. Gaponov ◽  
I.N. Mishustin

Open Physics ◽  
2010 ◽  
Vol 8 (4) ◽  
Author(s):  
Kaan Manisa ◽  
Ülfet Atav ◽  
Sibel Sarıaydın

AbstractA Variational Monte Carlo (VMC) method is employed to investigate the properties of symmetric and asymmetric nuclear matter. The realistic Urbana V 14 twonucleon interaction potential of Lagaris and Pandharipande was used to describe the microscopic interactions. Also, many body interactions are included as a density dependent term in the potential. Total kinetic and potential energies per particle are calculated for asymmetric nuclear matter by VMC method at various densities and isospin asymmetry parameters. The results are compared with data found in literature, and it was observed that the results obtained in this study reasonably agree with the results found in the literature. Also, the symmetry energy and incompressibility factor of the nuclear matter were obtained. The results obtained are in good agreement with those obtained by various authors with different methods and techniques.


2014 ◽  
Vol 77 (1) ◽  
pp. 100-109 ◽  
Author(s):  
V. K. Lukyanov ◽  
E. V. Zemlyanaya ◽  
K. V. Lukyanov ◽  
E. I. Zhabitskaya ◽  
M. V. Zhabitsky

1976 ◽  
Vol 14 (3) ◽  
pp. 1090-1101 ◽  
Author(s):  
L. S. Celenza ◽  
L. C. Liu ◽  
W. Nutt ◽  
C. M. Shakin

2012 ◽  
Vol 21 (09) ◽  
pp. 1250079 ◽  
Author(s):  
S. CHAKRABORTY ◽  
B. SAHOO ◽  
S. SAHOO

A phenomenological momentum dependent interaction (MDI) is considered to describe the equation of state (EOS) for isospin asymmetric nuclear matter (ANM), where the density dependence of the nuclear symmetry is the basic input. In this interaction, the symmetry energy shows soft dependence of density. Within the nonrelativistic mean field approach we calculate the nuclear matter fourth-order symmetry energy E sym, 4 (ρ). Our result shows that the value of E sym, 4 (ρ) at normal nuclear matter density ρ0( = 0.161 fm -3) is less than 1 MeV conforming the empirical parabolic approximation to the EOS of ANM at ρ0. Then the higher-order effects of the isospin asymmetry on the saturation density ρ sat (β), binding energy per nucleon K sat (β) and isobaric incompressibility K sat (β) of ANM is being studied, where [Formula: see text] is the isospin asymmetry. We have found that the fourth-order isospin asymmetry β cannot be neglected, while calculating these quantities. Hence the second-order K sat , 2 parameter basically characterizes the isospin dependence of the incompressibility of ANM at saturation density.


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