A self-consistent two-body method for three-body systems and the hypernucleus ΛBe9

1964 ◽  
Vol 56 ◽  
pp. 657-682 ◽  
Author(s):  
A.R. Bodmer ◽  
Shamsher Ali
2017 ◽  
Vol 26 (01n02) ◽  
pp. 1740025 ◽  
Author(s):  
J. Speth ◽  
N. Lyutorovich

Many-body Green functions are a very efficient formulation of the many-body problem. We review the application of this method to nuclear physics problems. The formulas which can be derived are of general applicability, e.g., in self-consistent as well as in nonself-consistent calculations. With the help of the Landau renormalization, one obtains relations without any approximations. This allows to apply conservation laws which lead to important general relations. We investigate the one-body and two-body Green functions as well as the three-body Green function and discuss their connection to nuclear observables. The generalization to systems with pair correlations are also presented. Numerical examples are compared with experimental data.


Pramana ◽  
2001 ◽  
Vol 57 (4) ◽  
pp. 701-716 ◽  
Author(s):  
Md Abdul Khan ◽  
Tapan Kumar Das

1965 ◽  
Vol 63 (4) ◽  
pp. 625-633 ◽  
Author(s):  
J.W. Murphy ◽  
S. Rosati

2013 ◽  
Vol 88 (5) ◽  
Author(s):  
Arianna Carbone ◽  
Andrea Cipollone ◽  
Carlo Barbieri ◽  
Arnau Rios ◽  
Artur Polls

2006 ◽  
Vol 15 (02) ◽  
pp. 346-353 ◽  
Author(s):  
N. PAAR ◽  
P. PAPAKONSTANTINOU ◽  
R. ROTH ◽  
H. HERGERT

The fully self-consistent Random Phase Approximation (RPA) is constructed within the Unitary Correlation Operator Method (UCOM), which describes the dominant interaction-induced short-range central and tensor correlations by a unitary transformation. Based on the correlated Argonne V18 interaction, the RPA is employed in studies of multipole response in closed-shell nuclei across the nuclide chart. The UCOM-RPA results in a collective character of giant resonances, and it describes rather well the properties of isoscalar giant monopole resonances. However, the excitation energies of isovector giant dipole resonances and isoscalar giant quadrupole resonances are overestimated due to the missing long-range correlations and three-body contributions.


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