In this study, the particle-vibration coupling for nuclei around 208Pb was taken into account. Then, Hamiltonian matrix in the basis of particle vibration eigenvectors was constructed and after matrix Diagonalization, fitting with experimental states was performed. Therefore, a set of pure single particle states was obtained which also called modified experimental levels. The results show that the neutron and proton energy gap were considerably increased to 0.81 MeV and 0.39 MeV in modified spectrum, respectively. The shell model parameters of phenomenological Woods-Saxon (WS) potential was then adjusted to reproduce these modified experimental states. The results showed that, WS potential with the help of new parameters predict the experim...
We calculate the single-particle resonances in a spherical Woods-Saxon potential using real stabiliz...
Single-particle spectra of spherical neutron-rich nuclei are studied. A Saxon-Wood's potential is us...
The new definition of the energy dependence for the level density parameter including collective eff...
The nucleon differential elastic scattering cross sections, the total proton reaction cross sections...
Positive-energy one-particle levels for neutrons in Y20 deformed Woods-Saxon potentials are examined...
We didcuss different approaches to the problem of reproducing the observed features of nuclear singl...
International audienceWe discuss different approaches to the problem of reproducing the observed fea...
The projected Woods-Saxon (WS) quasi-particle states have been used as the bases in the calculation ...
Initial results are presented for the determination of a global medium-energy nucleon-nucleus phenom...
Nuclear spectra of A = 14, 18, 38, 42, 206 and 208 nuclei were calculated using free reaction matric...
We present a computer program which solves the Schrodinger equation of the stationary states for an ...
Part I. The shell model near 208Pb. The nucleus 208Pb has a double closed shell of protons and neutr...
We calculate the single-particle resonances in a spherical Woods-Saxon potential using real stabiliz...
The properties of loosely bound proton-rich nuclei around A=20 are investigated within the framework...
Background: Nuclear shell model is widely applied in the studies of light and medium-mass nuclei. Th...
We calculate the single-particle resonances in a spherical Woods-Saxon potential using real stabiliz...
Single-particle spectra of spherical neutron-rich nuclei are studied. A Saxon-Wood's potential is us...
The new definition of the energy dependence for the level density parameter including collective eff...
The nucleon differential elastic scattering cross sections, the total proton reaction cross sections...
Positive-energy one-particle levels for neutrons in Y20 deformed Woods-Saxon potentials are examined...
We didcuss different approaches to the problem of reproducing the observed features of nuclear singl...
International audienceWe discuss different approaches to the problem of reproducing the observed fea...
The projected Woods-Saxon (WS) quasi-particle states have been used as the bases in the calculation ...
Initial results are presented for the determination of a global medium-energy nucleon-nucleus phenom...
Nuclear spectra of A = 14, 18, 38, 42, 206 and 208 nuclei were calculated using free reaction matric...
We present a computer program which solves the Schrodinger equation of the stationary states for an ...
Part I. The shell model near 208Pb. The nucleus 208Pb has a double closed shell of protons and neutr...
We calculate the single-particle resonances in a spherical Woods-Saxon potential using real stabiliz...
The properties of loosely bound proton-rich nuclei around A=20 are investigated within the framework...
Background: Nuclear shell model is widely applied in the studies of light and medium-mass nuclei. Th...
We calculate the single-particle resonances in a spherical Woods-Saxon potential using real stabiliz...
Single-particle spectra of spherical neutron-rich nuclei are studied. A Saxon-Wood's potential is us...
The new definition of the energy dependence for the level density parameter including collective eff...