invariant shell model
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2019 ◽  
Vol 222 ◽  
pp. 03027
Author(s):  
Yuriy Uzikov

The exclusive reaction 12C(p, ppN)10A of quasi-elastic knockout of the nucleon from the short-rangecorrelated nucleon pair <NN> in the 12C nucleus by proton with an energy of few GeV is considered in the plane-wave approximation.The two-nucleon spectroscopic factors and momentum distributions of the center of mass motion of NN-pairs are considered by analogy with theory of quasi-elastic knockout of fast deuteron clusters from nuclei (p, Nd) using the translationally-invariant shell model.


2016 ◽  
Vol 107 ◽  
pp. 10004
Author(s):  
R.V. Jolos ◽  
L. Majling ◽  
O. Majlingova

Open Physics ◽  
2013 ◽  
Vol 11 (5) ◽  
Author(s):  
Saulius Mickevičius ◽  
Darius Germanas ◽  
Ramutis Kalinauskas

AbstractA new procedure for large-scale calculations of the coefficients of fractional parentage (CFP) for many-particle systems is presented. The approach is based on a simple enumeration scheme for antisymmetric N particle states, and we suggest an efficient method for constructing the eigenvectors of two-particle transposition operator $$P_{N_1 ,N}$$ in a subspace where N 1 and N 2 = N − N 1 nucleons basis states are already antisymmetrized. The main result of this paper is that according to permutation operators $$P_{N_1 ,N}$$ eigenvalues we can distinguish totally asymmetrical N particle states from the other states with lower degree of asymmetry.


2005 ◽  
Vol 14 (02) ◽  
pp. 189-195 ◽  
Author(s):  
S. B. DOMA ◽  
ABDEL FATTAH M. EL-ZEBIDY

Two types of cluster–cluster potentials are obtained for the lithium nuclei. The first is an attractive one and the second is a superposition of repulsive and attractive Gaussian forces. The ground-state wave functions of the lithium nuclei 6 Li , 7 Li , 8 Li , and 9 Li are expanded in terms of products of two wave functions: the first represents the set of A-4 nucleons and the second represents the set of the last four nucleons. In the construction of these wave functions, we have used the basis functions of the translation-invariant shell model. The expansion coefficients of the factorizations of these wave functions are products of four-particle orbital and spin-isospin fractional parentage coefficients. Two least-square formulas for the cluster–cluster potentials, which depend on the mass number A, are fitted for the lithium nuclei.


1978 ◽  
Vol 34 (2) ◽  
pp. 173-183
Author(s):  
V. I. Ovcharenko ◽  
O. P. Pavlenko ◽  
G. F. Filippov

1970 ◽  
Vol 145 (2) ◽  
pp. 593-612 ◽  
Author(s):  
I.V. Kurdyumov ◽  
Yu.F. Smirnov ◽  
K.V. Shitikova ◽  
S.Kh.El. Samarai

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