Abstract
Absolute excitation functions for ($p, f$) reactions in ${\mathrm{Th}}^{232}$, ${\mathrm{U}}^{235}$, and ${\mathrm{U}}^{238}$ were measured by radiochemical techniques; at 21.5 Mev, the cross sections are 0.83, 1.31, and 1.28 barns, respectively (\ifmmode\pm\else\textpm\fi{}15 percent in each case). Cross sections for ($p, \mathrm{xn}$) reactions in ${\mathrm{U}}^{238}$ were found to be quite small. The total reaction cross sections correspond to a nuclear radius of $(1.55\ifmmode\pm\else\textpm\fi{}0.1){\mathrm{A}}^{\frac{1}{3}}\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}13}$ cm. Some advantages of determining the nuclear radius by total reaction cross sections are pointed out, and the discrepancy between electromagnetic and nuclear determinations of the nuclear radius is discussed.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.