  We analyze various possible interpretations of the narrow state
$D_{sJ}(2632)$ which lies 100 MeV above threshold. This interesting state
decays mainly into $D_s \eta$ instead of $D^0 K^+$. If this relative branching
ratio is further confirmed by other experimental groups, we point out that the
identification of $D_{sJ}(2632)$ either as a $c\bar s$ state or more generally
as a ${\bf {\bar 3}}$ state in the $SU(3)_F$ representation is probably
problematic. Instead, such an anomalous decay pattern strongly indicates
$D_{sJ}(2632)$ is a four quark state in the $SU(3)_F$ ${\bf 15}$ representation
with the quark content ${1\over 2\sqrt{2}}
(ds\bar{d}+sd\bar{d}+su\bar{u}+us\bar{u}-2ss\bar{s})\bar{c}$. We discuss its
partners in the same multiplet, and the similar four-quark states composed of a
bottom quark $B_{sJ}^0(5832)$. Experimental searches of other members
especially those exotic ones are strongly called for.
