  The LHCb Collaboration has recently reported the observation for the first
time of a spin-$3$ resonance in the heavy quark sector. They have shown that
the $\bar{D}^{0}K^{-}$ structure seen in the $B_{s}^{0}\to
\bar{D}^{0}K^{-}\pi^{+}$ reaction and with invariant mass $2.86\,{\rm GeV}$ is
an admixture of a spin-$1$ and a spin-$3$ resonances. Motivated by the good
agreement between our theoretical predictions some time ago and the properties
extracted from the experiment of the $D_{s1}^{\ast}(2860)$ and
$D_{s3}^{\ast}(2860)$ states, we perform an extension of the study of the
strong decay properties of the $D_{sJ}^{\ast}(2860)$ and present the same
analysis for the $D_{s1}^{\ast}(2700)$ and $D_{sJ}(3040)$ mesons. This provides
a unified and simultaneous description of the three higher excited
charmed-strange resonances observed until now. For completeness, we present
theoretical results for masses and strong decays of the low-lying
charmed-strange mesons and those experimental missing states which belong to
the spin-multiplets of the discovered $D_{s1}^{\ast}(2700)$,
$D_{sJ}^{\ast}(2860)$ and $D_{sJ}(3040)$ resonances. The theoretical framework
used is a constituent quark model which successfully describes hadron
phenomenology from light to heavy quark sectors.
