Interplay between single-particle and collective degrees of freedom in the excitation of the low-lying states in 140Ce.

Abstract

Differential cross sections for electron scattering from $^{140}\mathrm{Ce}$ have been measured for excitation energies less than 3.3 MeV over a range of effective momentum transfer of 0.4 to 3.1 ${\mathrm{fm}}^{\mathrm{\ensuremath{-}}1}$. The data have been analyzed to extract transition charge densities. These densities are interpreted in terms of a quasiparticle-phonon model and self-consistent finite Fermi system theory to disentangle the collective and noncollective modes of excitation.