  In this work, we preform a systematic study of the strong decays for the
higher singly heavy baryon resonances $\Lambda_Q(3S)$, $\Lambda_Q(2P)$,
$\Lambda_Q(2D)$, $\Lambda_Q(1F)$, $\Sigma_Q(3S)$, $\Sigma_Q(2P)$,
$\Sigma_Q(2D)$, and $\Sigma_Q(1F)$ within the $^3P_0$ model. Our results show
that most of the $\lambda-$mode higher excited $\Lambda_Q$ and $\Sigma_Q$
states have a relatively narrow width, and mainly decay into two-body final
states with one heavy meson plus one light baryon. Our calculations provide
abundant theoretical information and demonstrate the general feature for these
higher states, which may be valuable for future experimental searches and
establishing the singly heavy baryon spectrum.
