High-Resolution Studies of (d,p) Reactions onCd114andIn115

Energy and angular distributions from 12-MeV deuteron-induced ($d,p$) reactions on ${\mathrm{Cd}}^{114}$ and ${\mathrm{In}}^{115}$ were measured with ∼8-keV energy resolution. In ${\mathrm{In}}^{115}\mathrm{}(d,p)\mathrm{}$ essentially all components of the ($\pi g_{\frac{9}{2}}^{}{}_{}{}^{-1\mathrm{}}$) ($\nu h_{\frac{11}{2}}$) configuration are located, and $I$ values are estimated from sum rules. $I$ values for many members of the ($\pi g_{\frac{9}{2}}^{}{}_{}{}^{-1\mathrm{}}$) ($\nu d_{\frac{3}{2}}$) and ($\pi g_{\frac{9}{2}}^{}{}_{}{}^{-1\mathrm{}}$) ($\nu s_{\frac{1}{2}}$) are determined from sum rules and the presence or absence of $l=0\mathrm{}$ and $l=2\mathrm{}$ mixing. As in a previous study of $\mathrm{Pd}\mathrm{}(d,p)\mathrm{}$, there is a large excess of $g_{\frac{7}{2}}$ and a large deficiency of $h_{\frac{11}{2}}$ strength relative to the isotonic tin nucleus (${\mathrm{Sn}}^{116}$) and expectations from nuclear-structure theory. The most obvious experimental explanations for this discrepancy are discussed and found not to be applicable.