Abstract
Results are presented concerning theoretical predictions of existence of hyperdeformed high spin states for nuclei with 58{<=}Z{<=}92 and for more than 10 isotopes for each element (only even-even nuclei). The calculations were based on the cranking method and Strutinsky`s shell correction. The following were taken as the two most important criteria for the possible existence of hyperdeformed states: the energy of the hyperdeformed state relative to the yrast line, and the minimum height of the barrier separating the hyperdeformed minimum from normal states and from fission. 15 refs., 4 figs.
Werner, T R;
[1]
Dudek, J
[2]
- Institute of Theoretical Physics, Warsaw (Poland)
- Strasbourg-1 Univ., 67 (France). Centre de Recherches Nucleaires
Citation Formats
Werner, T R, and Dudek, J.
Where to look for hyperdeformed states.
Canada: N. p.,
1992.
Web.
Werner, T R, & Dudek, J.
Where to look for hyperdeformed states.
Canada.
Werner, T R, and Dudek, J.
1992.
"Where to look for hyperdeformed states."
Canada.
@misc{etde_520603,
title = {Where to look for hyperdeformed states}
author = {Werner, T R, and Dudek, J}
abstractNote = {Results are presented concerning theoretical predictions of existence of hyperdeformed high spin states for nuclei with 58{<=}Z{<=}92 and for more than 10 isotopes for each element (only even-even nuclei). The calculations were based on the cranking method and Strutinsky`s shell correction. The following were taken as the two most important criteria for the possible existence of hyperdeformed states: the energy of the hyperdeformed state relative to the yrast line, and the minimum height of the barrier separating the hyperdeformed minimum from normal states and from fission. 15 refs., 4 figs.}
place = {Canada}
year = {1992}
month = {Aug}
}
title = {Where to look for hyperdeformed states}
author = {Werner, T R, and Dudek, J}
abstractNote = {Results are presented concerning theoretical predictions of existence of hyperdeformed high spin states for nuclei with 58{<=}Z{<=}92 and for more than 10 isotopes for each element (only even-even nuclei). The calculations were based on the cranking method and Strutinsky`s shell correction. The following were taken as the two most important criteria for the possible existence of hyperdeformed states: the energy of the hyperdeformed state relative to the yrast line, and the minimum height of the barrier separating the hyperdeformed minimum from normal states and from fission. 15 refs., 4 figs.}
place = {Canada}
year = {1992}
month = {Aug}
}