  It is shown that in the framework of GIM model,the parity-violating (PV)
$\Sigma^{+}(uus) \Rightarrow p(uud) + \gamma $ decay amplitude does not vanish
but just transforms into another PV decay amplitude, namely, of the
$\Omega^{+}_{cc}(ccs)\to \Xi^{+}_{cc}(ccd)+\gamma $ decay. The known result is
used that the relevant part of the CP-invariant effective current$\times$
current Hamiltonian changes sign under simultaneous quark changes
$d\leftrightarrow s$ and $u\leftrightarrow c$. So, asymmetry of $\Sigma^{+}
\Rightarrow p + \gamma $ decay should not vanish in contrast to the Hara result
of the old-fashioned $SU(3)_{f}$ model. At the same time, the zero asymmetry
prediction persists for the $ \Xi^{-} \Rightarrow \Sigma^{-} + \gamma $ decay.
