The relation between di-neutron cluster model and shell model configurations in 11Li

1991 ◽  
Vol 254 (1-2) ◽  
pp. 15-19 ◽  
Author(s):  
A.C. Hayes
2009 ◽  
Vol 24 (11) ◽  
pp. 2091-2100 ◽  
Author(s):  
TOSHIO MOTOBA

Prospects of interesting hypernuclear structures are discussed for typical light p-shell systems with the cluster model application and also for the medium-heavy systems with shell-model applications. Corresponding to the recent experimental progress, importance of production reaction spectroscopy are emphasized.


2007 ◽  
Vol 75 (6) ◽  
Author(s):  
A. M. Moro ◽  
K. Rusek ◽  
J. M. Arias ◽  
J. Gómez-Camacho ◽  
M. Rodríguez-Gallardo

1997 ◽  
Vol 620 (1) ◽  
pp. 29-45 ◽  
Author(s):  
N.K. Timofeyuk ◽  
D. Baye ◽  
P. Descouvemont

2011 ◽  
Vol 20 (04) ◽  
pp. 1022-1025
Author(s):  
MARIANNE DUFOUR ◽  
PIERRE DESCOUVEMONT

This work is devoted to a Generator-Coordinate-Method investigation of the 16 B spectrum with an Extended Two-Cluster Model which includes many 15 B + n channels. We find that the narrow peak above the 15 B + n threshold seen in the experiments of Kalpachieva et al. and of Lecouey et al. can be assigned to a [Formula: see text] resonance. Several resonances are obtained near the 15 B + n threshold, in particular a [Formula: see text] state which could be a possible candidate for the 16 B ground state. Comparison with Shell Model calculations is performed.


2009 ◽  
Vol 18 (01) ◽  
pp. 183-192
Author(s):  
MOHAMED AHMED HASSAN

A numerical representation for nuclei is suggested and considered as a basis of a cluster model. The binding energy of the cluster representation of a nucleus is introduced. Basic assumptions of the shell model are obtained as the physical side of the suggested cluster representation. 8 Be 4-decay to two α-particles and 9 B 5 decay to two α-particles and proton are interpreted.


2020 ◽  
Vol 15 (1) ◽  
Author(s):  
Neelam Sinha ◽  
Piyush Sinha

In this paper cluster model wave function for 6Li using Shell Model with definite parity and angular momentum is written along with cluster co-ordinates, which are relative to the center-of-mass of various clusters and involve with parameters. These parameters can be adjusted to some extent to obtain predictions close to experimental properties. The cluster model wave function is written along with resonating group method (RGM) and the Complex Generator Coordinate Technique (CGCT). The Complex Generator Coordinate Technique allows the transformation of the cluster model wave function written in terms of cluster co-ordinates into anti-symmetrized product of single particle wave function. This wave function is written in terms of single particle co-ordinates, the center-of-mass co-ordinates, parameter coordinates and generator coordinates.


2020 ◽  
Vol 98 (1) ◽  
pp. 28-31 ◽  
Author(s):  
Zari Binesh ◽  
Mohammad Reza Shojaei ◽  
Behnam Azadegan

In this paper, we study the 9B and 9Be mirror nuclei with shell and cluster models. The modified Eckart plus Coulomb repulsive potentials are selected to describe the interaction between particles. By solving the Schrödinger equation, the exact solution of this equation is obtained by the parametric Nikiforov–Uvarov (PNU) method. The eigenvalues and wave function are calculated for 9B and 9Be. Our results are compared with experimental results, as well as results from other papers, and are in good agreement.


2021 ◽  
Vol 14 (4) ◽  
pp. 333-338

Abstract: In this paper, we have investigated electric quadrupole moment of (_^6)Li and (_^7)Li in both shell model and cluster model. In shell model, the nuclei (_^6)Li and (_^7)Li can be modeled as one core plus nucleons. Nucleons outside the closed shell can be considered as a two- and three-particle system. In cluster structure, we have selected alpha clusters and triton or deuteron in interaction with alpha cluster ((_^7)Li and (_^6)Li involving α+(_^3)H and α+(_^2)H, respectively). By solving Schrödinger equation and using suitable potential for interaction between particles by applying Nikiforov-Uvarov method, potential coefficients have been computed. Then, we have calculated the energy and wave function for nuclei(_^6)Li and (_^7)Li and compared the results obtained with experimental results. By having the wave function, we can obtain the quadrupole moment. These values are compared with predictions from shell-model and cluster-model calculations. Although the difference between them is small, the electric quadrupole moment results in the cluster model are in good agreement with experimental results. Keywords: Electric quadrupole moment, Shell-model, Cluster-model, Li isotopes, Non-relativistic equation.


Sign in / Sign up

Export Citation Format

Share Document