Remeasuring the Anomalously Enhanced B(E2;2+→1+) in Li

The large reported $E2$ strength between the ${2}^{+}$ ground state and ${1}^{+}$ first excited state of $^{8}\mathrm{Li}, B(E2;{2}^{+}\ensuremath{\rightarrow}{1}^{+})=55(15)\phantom{\rule{4pt}{0ex}}{e}^{2}{\mathrm{fm}}^{4}$, presents a puzzle. Unlike in neighboring $A=7--9$ isotopes, where enhanced $E2$ strengths may be understood to arise from deformation as rotational in-band transitions, the ${2}^{+}\ensuremath{\rightarrow}{1}^{+}$ transition in $^{8}\mathrm{Li}$ cannot be understood in any simple way as a rotational in-band transition. Moreover, the reported strength exceeds ab initio predictions by an order of magnitude. In light of this discrepancy, we revisited the Coulomb excitation measurement of this strength, now using particle-$\ensuremath{\gamma}$ coincidences, yielding a revised $B(E2;{2}^{+}\ensuremath{\rightarrow}{1}^{+})$ of $19{(}_{\ensuremath{-}6}^{+7})(2)\phantom{\rule{4pt}{0ex}}{e}^{2}{\mathrm{fm}}^{4}$. We explore how this value compares to what might be expected in the limits of rotational models. While the present value is about a factor of three smaller than previously reported, the current experimental data indicates that the $B(E2)$ value remains anomalously enhanced.