  The magnetic moment - a function of the electric charge form factor
$F_{1}(q^{2})$ and the magnetic dipole form factor $F_{2}(q^{2})$ at zero
four-momentum transfer $q^{2}$-of the ground-state $J^{P}=(3/2)^{+}$ baryon
decuplet magnetic moments have been studied for many years with limited
success. At present, only the magnetic moment of the $\Omega^{-}$ has been
accurately determined. We calculate nonperturbatively the magnetic moments of
the \emph{physical baryon decuplet $J^{P}=(3/2)^{+}$} members and in
particular, we obtain $\mu_{\Delta^{++}}= (+3.67 \pm 0.07) \mu_{N}$,
$\mu_{\Delta^{+}}= (+1.83 \pm 0.04) \mu_{N}$, $\mu_{\Delta^{0}}= (0) \mu_{N}$,
and the magnetic moments of their $U$-Spin partners in terms of $\Omega^{-}$
magnetic moment data.
