How good is a Jastrow trial wave function for nuclear matter?

1976 ◽  
Vol 65 (5) ◽  
pp. 405-408 ◽  
Author(s):  
M.L. Ristig ◽  
P. Hecking
2000 ◽  
Vol 62 (12) ◽  
pp. 8171-8179 ◽  
Author(s):  
S.-R. Eric Yang ◽  
Min-Chul Cha ◽  
Jung Hoon Han

1970 ◽  
Vol 153 (1) ◽  
pp. 172-182 ◽  
Author(s):  
H. Hutzelmeyer

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.


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