Excitation functions have been measured for the production of fission isomers by (α,xn) reactions for bombarding energies of 20-29 MeV and by ($d,2n$), ($d,p$), and ($d,pn$) reactions for bombarding energies of 9-14 MeV. Excitation functions for (α,xn) reactions were measured for targets of ²³³U, ²³⁴U, ²³⁵U, ²³⁶U, ²³⁸U, ²³⁷Np, ²³⁹Pu, ²⁴⁰Pu, ²⁴²Pu, and ²⁴⁴Pu. Excitation functions for deuteron reactions were measured for targets of ²³⁵U, ²³⁷Np, ²³⁹Pu, ²⁴⁰Pu, ²⁴²Pu, ²⁴⁴Pu, and ²⁴³Am. New or more accurate half-lives were determined for the following fission isomers: ²³⁵ᵐPu, 30 ±{} 5 nsec; ²³⁸ᵐPu, 6.5 ±{} 1 nsec; ²⁴⁰ᵐPu, 3.8 ±{} 0.3 nsec; ²⁴¹ᵐCm, 15.3 ±{} 1 nsec; and ²⁴⁵ᵐCm, 23 ±{} 5 nsec. Isomers in ²⁴²Cm and ²⁴⁴Cm were identified but their half-lives were too long for measurement with the present techniques. The results are analyzed with a statistical model using realistic level-density expressions with many parameters fixed by comparison with experimental measurements of neutron-fission cross sections, neutron-to-fission decay widths, spallation cross sections, and fission lifetimes. This model is applied to the presently measured excitation functions and the results obtained previously by other groups for ($n,2n$), ($p,2n$), and (γ,n) reactions. With this model fission-barrier parameters are determined for Pu, Am, and Cm isotopes. Inconsistencies in the results obtained by applying this model to experimental isomer excitation functions indicate the directions for future refinements.
No takes yet. Share an insight, caveat, or question.
Britt et al. (1971) studied this question.
Synapse has enriched one closely related paper. Consider it for comparative context: