The collective yrast band and the high spin states of the nucleus 50Cr are studied using the spherical shell model and the HFB method. The two descriptions lead to nearly the same values for the relevant observables. A first backbending is predicted at I=10\hbar corresponding to a collective to non-collective transition. At I=16\hbar a second backbending occurs, associated to a configuration change that can also be interpreted as an spherical to triaxial transition
One of the goals pursued in the present research was to understand the nuclear phenomena (such as ro...
AbstractExcited states up to Iπ=8+ in the neutron-rich nucleus 58Cr have been identified by using a ...
The formalism of the neutron-photon interacting boson model, extended to include two-quasiparticle e...
ReVTeX v 3.0 epsf.sty, 5 pages, 5 figures included. Full Postscript version available at http://www....
Gamma rays from the N = Z-2 nucleus (50)Fe have been observed, establishing the rotational ground st...
We provide new insights into backbending phenomenon within the symmetry-adapted framework which natu...
The backbending phenomena observed in Ce isotopes, 132,134,136Ce are investigated in terms of a pair...
Gamma rays from the N = Z-2 nucleus 50Fe have been observed, establishing the rotational ground stat...
Gamma rays from the N = Z - 2 nucleus Fe-50 have been observed, establishing the rotational ground s...
The oscillating behaviour of backbending due the rotational alignment of two i13/2 neutrons is expla...
A theoretical interpretation of the reduction in E2 strengths in 126Ba prior to backbending is prese...
DSAM lifetimes have been determined in the middle of 1f7/2 shell for the cross-conjugated nuclei 47 ...
The yrast line of the N=Z nucleus 48Cr is studied up to high spins by means of the cranked Hartree-F...
Excited states up to Iπ = 8+ in the neutron-rich nucleus 58Cr have been identified by using a new ex...
The yrast line of the N=Z nucleus 48Cr is studied up to high spins by means of the cranked Hartree-F...
One of the goals pursued in the present research was to understand the nuclear phenomena (such as ro...
AbstractExcited states up to Iπ=8+ in the neutron-rich nucleus 58Cr have been identified by using a ...
The formalism of the neutron-photon interacting boson model, extended to include two-quasiparticle e...
ReVTeX v 3.0 epsf.sty, 5 pages, 5 figures included. Full Postscript version available at http://www....
Gamma rays from the N = Z-2 nucleus (50)Fe have been observed, establishing the rotational ground st...
We provide new insights into backbending phenomenon within the symmetry-adapted framework which natu...
The backbending phenomena observed in Ce isotopes, 132,134,136Ce are investigated in terms of a pair...
Gamma rays from the N = Z-2 nucleus 50Fe have been observed, establishing the rotational ground stat...
Gamma rays from the N = Z - 2 nucleus Fe-50 have been observed, establishing the rotational ground s...
The oscillating behaviour of backbending due the rotational alignment of two i13/2 neutrons is expla...
A theoretical interpretation of the reduction in E2 strengths in 126Ba prior to backbending is prese...
DSAM lifetimes have been determined in the middle of 1f7/2 shell for the cross-conjugated nuclei 47 ...
The yrast line of the N=Z nucleus 48Cr is studied up to high spins by means of the cranked Hartree-F...
Excited states up to Iπ = 8+ in the neutron-rich nucleus 58Cr have been identified by using a new ex...
The yrast line of the N=Z nucleus 48Cr is studied up to high spins by means of the cranked Hartree-F...
One of the goals pursued in the present research was to understand the nuclear phenomena (such as ro...
AbstractExcited states up to Iπ=8+ in the neutron-rich nucleus 58Cr have been identified by using a ...
The formalism of the neutron-photon interacting boson model, extended to include two-quasiparticle e...