  We have evaluated the strong decays of the $K_0^*(1950)$ and $K_0^*(2130)$
within the $^3P_0$ model, by employing the meson wave functions from the
relativized quark model. By comparing with the experimental measurements, the
$K_0^*(2130)$ could be assigned as $K_0^*(3^3P_0)$, while the $K_0^*(1950)$
seems like an exotic state, because its width can not be reasonably reproduced
within the $^3P_0$ model. We also predict that the $K_0^*(2^3P_0)$ state has a
mass of about $1811$ MeV and a width of about $656$ MeV, while the
$K_0^*(4^3P_0)$ state has a mass of about $2404$ MeV and a width of about $180$
MeV.
