Variation in Nuclear-Matter Binding Energies with Phase-Shift-Equivalent Two-Body Potentials

1970 ◽  
Vol 1 (3) ◽  
pp. 769-776 ◽  
Author(s):  
F. Coester ◽  
S. Cohen ◽  
B. Day ◽  
C. M. Vincent
1972 ◽  
Vol 5 (3) ◽  
pp. 1135-1136 ◽  
Author(s):  
F. Coester ◽  
B. Day ◽  
A. Goodman

2006 ◽  
Vol 15 (02) ◽  
pp. 339-345 ◽  
Author(s):  
F. CHAPPERT ◽  
M. GIROD

A new parameterization of the effective Gogny interaction is investigated. It has the property of fitting the neutron matter Equation Of State (EOS) as predicted by a variational calculation. Its properties in nuclear matter (saturation point, compressibility, …) and in nuclei (binding energies) are presented.


1976 ◽  
Vol 54 (22) ◽  
pp. 2225-2239 ◽  
Author(s):  
R. J. W. Hodgson ◽  
J. Tan

The fully off-shell T matrix is generated from a real symmetric function σ(k,k′) which in turn can be obtained from a knowledge of the two-body wave function in the interaction interior. The resulting T matrices are employed to compute the binding energies of 16O, 40Ca, and nuclear matter. Limiting the two-body wave function to physically acceptable forms limits the allowed σ functions. A 'difference integral' is defined in terms of the two-body scattering wave function, which seems to be strongly correlated with the binding energies.


1975 ◽  
Vol 242 (3) ◽  
pp. 467-480 ◽  
Author(s):  
Sidney A. Coon ◽  
Michael D. Scadron ◽  
Bruce R. Barrett

1972 ◽  
Vol 50 (14) ◽  
pp. 1614-1618 ◽  
Author(s):  
N. N. Wong ◽  
M. Razavy

A two-body transparent potential, which produces no observable phase shift in two-particle scattering, is constructed explicitly. This potential is used to calculate the energy of infinite nuclear matter by applying the perturbation theory and its effects on the many-body system are investigated.


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