  We have used realistic local interactions based on the recent update of the
strangeness $-2$ Nijmegen ESC08c potential to calculate the bound state problem
of the $\Xi NN$ system in the $(I)J^P=(\frac{1}{2})\frac{3}{2}^+$ state. We
found that this system presents a deeply bound state lying $13.5$ MeV below the
$\Xi d$ threshold. Since in lowest order, pure S$-$wave configuration, this
system can not decay into the open $\Lambda\Lambda N$ channel, its decay width
is expected to be very small. We have also recalculated the
$(I)J^P=(\frac{3}{2})\frac{1}{2}^+$ state and we have compared with results of
quark-model based potentials.
