The mean square spin value of the compound nucleus $^{248}\mathrm{Cf}$ has been determined from fissionfragment angular distributions for the $^{12}\mathrm{C}$ + $^{236}\mathrm{U}$ and $^{16}\mathrm{O}$ + $^{232}\mathrm{Th}$ reactions. The anisotropy and, hence, the mean square spin values are much larger than expected. Models which reproduce the enhancement observed in the sub-barrier fusion excitation functions fail to account for the spin-distribution observations.
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