A theoretical interpretation of the reduction in E2 strengths in 126Ba prior to backbending is presented. A shell model basis is built from normal parity orbilals organized into multiplets of a pseudo SU(3) symmetry coupled to h 11 2 configurations restricted to states of seniority zero and two. Within the framework of the model the scattering of a pair of protons from normal parity to the h 11 2 orbital produces band crossing and a corresponding reduction in E2 transition strengths prior to pair alignment which is the principal mechanism of the backbending. © 1981
In terms of the exaxt angular momentum projection, properties of the three dimensional cranked HFB (...
International audienceThree new negative-parity bands have been identified in Ba120, two of them for...
It is shown that, in some cases, the back-bending phenomenon in the energy levels of even-even defor...
A theoretical interpretation of the reduction in E2 strengths in 126Ba prior to backbending is prese...
Lifetimes of 17 levels of 124Xe were measured using the Recoil Distance Doppler Shift method. An ano...
The backbending phenomena observed in Ce isotopes, 132,134,136Ce are investigated in terms of a pair...
Using two Compton-suppression spectrometers in an Eγ−Eγ coincidence experiment, the yrast bands in 1...
Interband B(E2) transition strengths between different normal parity bands in 163Dy and 165Er are de...
The decoupled h11/2 bands in Au nuclei are investigated in the framework of a shell model descriptio...
The oscillating behaviour of backbending due the rotational alignment of two i13/2 neutrons is expla...
The collective yrast band and the high spin states of the nucleus 50Cr are studied using the spheric...
Garrett et al. systematically investigated band-crossing frequencies resulting from the rotational a...
We provide new insights into backbending phenomenon within the symmetry-adapted framework which natu...
In two recent publications by Broglia et al. (see Phys. Lett., vol.57B, p.113 (1975)), it has been s...
Using a simple model for low-lying positive-parity resonances in 13Be as 10Be x (sd)3 and 12Be1p x (...
In terms of the exaxt angular momentum projection, properties of the three dimensional cranked HFB (...
International audienceThree new negative-parity bands have been identified in Ba120, two of them for...
It is shown that, in some cases, the back-bending phenomenon in the energy levels of even-even defor...
A theoretical interpretation of the reduction in E2 strengths in 126Ba prior to backbending is prese...
Lifetimes of 17 levels of 124Xe were measured using the Recoil Distance Doppler Shift method. An ano...
The backbending phenomena observed in Ce isotopes, 132,134,136Ce are investigated in terms of a pair...
Using two Compton-suppression spectrometers in an Eγ−Eγ coincidence experiment, the yrast bands in 1...
Interband B(E2) transition strengths between different normal parity bands in 163Dy and 165Er are de...
The decoupled h11/2 bands in Au nuclei are investigated in the framework of a shell model descriptio...
The oscillating behaviour of backbending due the rotational alignment of two i13/2 neutrons is expla...
The collective yrast band and the high spin states of the nucleus 50Cr are studied using the spheric...
Garrett et al. systematically investigated band-crossing frequencies resulting from the rotational a...
We provide new insights into backbending phenomenon within the symmetry-adapted framework which natu...
In two recent publications by Broglia et al. (see Phys. Lett., vol.57B, p.113 (1975)), it has been s...
Using a simple model for low-lying positive-parity resonances in 13Be as 10Be x (sd)3 and 12Be1p x (...
In terms of the exaxt angular momentum projection, properties of the three dimensional cranked HFB (...
International audienceThree new negative-parity bands have been identified in Ba120, two of them for...
It is shown that, in some cases, the back-bending phenomenon in the energy levels of even-even defor...