The yields of gamma rays resulting from Coulomb excitation have been measured for Tl²⁰⁵, Tl²⁰³, Au¹⁹⁷, Ir¹⁹³, Ir¹⁹¹, Re¹⁸⁷, Re¹⁸⁵, W¹⁸³, Ta¹⁸¹, Cd¹¹³, Cd¹¹¹, Ag¹⁰⁹, Ag¹⁰⁷, Rh¹⁰³, Mo⁹⁵, Os¹⁹², Os¹⁹⁰, Os¹⁸⁸, W¹⁸⁶, W¹⁸⁴, and W¹⁸². Angular distributions of the gamma radiation from the nuclei Tl²⁰⁵, Tl²⁰³, Au¹⁹⁷, Ir¹⁹³, Ir¹⁹¹, Re¹⁸⁷, Re¹⁸⁵, Ta¹⁸¹, Cd¹¹³, Cd¹¹¹, Ag¹⁰⁹, Ag¹⁰⁷, Rh¹⁰³, and Mo⁹⁵ have been measured with respect to the incident proton beam on thick targets. The linear polarization of gamma rays following Coulomb excitation has been studied. A polarimeter based on the Compton scattering mechanism has been constructed and its effectiveness determined by measurements of the known polarization of gamma rays from excitation of 2+ levels in even-even nuclei. Polarization-direction measurements of several transitions in odd-mass nuclei have resolved the ambiguity either in the value of (E2/M1)1/2 or in the spin of the excited state deduced from the angular distributions. Reduced transition probabilities for $E2$ and $M1$ transitions are obtained. In some instances these quantities are compared to the predictions of the collective model of the nucleus.
No takes yet. Share an insight, caveat, or question.
McGowan et al. (1958) studied this question.
Synapse has enriched 5 closely related papers on similar clinical questions. Consider them for comparative context: