Abstract

A coupled-channel calculation including Coulomb excitation has been done for excitation of the isovector giant dipole resonance in light-ion inelastic scattering from $^{208}\mathrm{Pb}$ at forward angles. It is found that the predicted cross sections for excitation of the giant dipole resonance with alpha inelastic scattering, calculated including Coulomb excitation, are much smaller than the experimental isoscalar giant monopole resonance cross section at incident energies around 100 MeV. The predicted cross section for Coulomb excitation of the giant dipole resonance increases rapidly with increasing incident energy, and the giant dipole and monopole resonance cross sections become comparable above ${E}_{\ensuremath{\alpha}}=300$ MeV. For inelastic scattering of $^{3}\mathrm{He}$, deuterons, and protons at forward angles, Coulomb excitation of the giant dipole resonance is found to be comparable to the giant monopole resonance cross section at $100l{E}^{\mathrm{lab}}l200$ MeV. Coulomb excitation of the giant dipole resonance is strongly inhibited by momentum mismatch between incident and outgoing waves due to the large negative $Q$ values. This mismatch is reduced for lighter projectile masses and higher incident energies. As the giant monopole and dipole resonances are almost coincident, giant dipole resonance excitation must be properly accounted for in studies of the giant monopole resonance.NUCLEAR REACTIONS Coupled-channel calculation of $\ensuremath{\sigma}(\ensuremath{\theta})$; for Coulomb excitation of isovector dipole resonance in $^{208}\mathrm{Pb}$; from ($\ensuremath{\alpha}$,${\ensuremath{\alpha}}^{\ensuremath{'}}$), ($^{3}\mathrm{He}$, $^{3}\mathrm{He}$'), ($d$,${d}^{\ensuremath{'}}$), and ($p$,${p}^{\ensuremath{'}}$) scattering.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

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.