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Initial versions of some panels in Figs. 7, 8, and 9 contained narrow oscillations which were computational artifacts, due to incomplete convergence of selected state-to-state transition probabilities when the total energy nearly coincides with the opening of a new channel. These could in principle be avoided by an especially careful convergence protocol, but here the problematic data were deleted before spline fitting to obtain the DORS or state-selected DORS. The omitted energies follow. For Fig. 7, the JPS = 6+ + DORS panel, 0.70, 0.82, 0.93, and 1.03 eV. For Fig. 8(b), v = 0, and Fig. 9, left JPS = 3 - + panels, 1.16 eV. For Fig. 8(c), v = 0 and v′ = 0 and Fig. 9, JPS = 9 - + panels, 1.22 eV. For Fig. 9, left JPS = 6+ + panel, 0.93 eV. For Fig. 9, right JPS = 6+ + panel, 0.70, 0.82, 0.93, 1.03, and 1.09 eV.
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