English (United Kingdom)

https://curated-unify.zendy.io/wp-json/zendy-region/v1/featured_content/oa?rat=en

https://curated-unify.zendy.io/wp-json/zendy-region/v1/highlighted_journal/

Global: Zendy Plus annual

Presents the access of premium content as premium feature

Premium Content

Presents the keyphrase highlighting as premium feature

Keyphrase Highlighting

Presents the summarisation as premium feature

Summarisation

Insights

Presents the pdf analysis as premium feature

PDF Analysis

Presents the zaia usage as premium feature

ZAIA

Global: Zendy Tools annual

Global: Zendy Free Plan

Global: Zendy Tools monthly

Global: Zendy Plus monthly

The fission probability of 232Pa was measured as a function of the excitationenergy in order to search for hyperdeformed (HD) transmission resonances usingthe (d,pf) transfer reaction on a radioactive 231Pa target. The experiment wasperformed at the Tandem accelerator of the Maier-Leibnitz Laboratory (MLL) atGarching using the 231Pa(d,pf) reaction at a bombarding energy of E=12 MeV andwith an energy resolution of dE=5.5 keV. Two groups of transmission resonanceshave been observed at excitation energies of E=5.7 and 5.9 MeV. The finestructure of the resonance group at E=5.7 MeV could be interpreted asoverlapping rotational bands with a rotational parameter characteristic to a HDnuclear shape. The fission barrier parameters of 232Pa have been determined byfitting TALYS 1.2 nuclear reaction code calculations to the overall structureof the fission probability. From the average level spacing of the J=4 states,the excitation energy of the ground state of the 3rd minimum has been deducedto be E(III)=5.05 MeV.

Transmission resonance spectroscopy in the third minimum of 232Pa