  The spectra and decay rates of $c \bar c$ and $b \bar b$ levels are well
described, for the most part, by a power-law potential of the form
$V(r)=\lambda(r^{\alpha}-1)/\alpha+{\rm const.}$, where $\alpha\simeq 0$. The
results of an up-to-date fit to the data on spin-averaged levels are presented.
Results on electric dipole transitions in systems bound by power law potentials
are also presented, with applications to the bottomonium system.
