  Based on $e^{+}e^{-}$ collision data collected at center-of-mass energies
from 2.000 to 3.080 GeV by the BESIII detector at the BEPCII collider, a
partial wave analysis is performed for the process $e^{+}e^{-}\to K_{S}^{0}
K_{L}^{0} \pi^{0}$. The results allow the Born cross sections of the process
$e^{+}e^{-}\to K_{S}^{0} K_{L}^{0} \pi^{0}$, as well as its subprocesses
$e^{+}e^{-}\to K^{*}(892)^{0}\bar{K}^{0}$ and $K^{*}_{2}(1430)^{0}\bar{K}^{0}$
to be measured. The Born cross sections for $e^{+}e^{-}\to
K_{S}^{0}K_{L}^{0}\pi^{0}$ are consistent with previous measurements by BaBar,
but with substantially improved precision. The Born cross section lineshape of
the process $e^{+}e^{-}\to K^{*}(892)^{0}\bar{K}^{0}$ is consistent with a
vector meson state around 2.2 GeV with a significance of 3.2$\sigma$. A
Breit-Wigner fit determines its mass as
$M_Y=(2164.7\pm9.1\pm3.1)~{\rm{MeV}}/c^{2}$ and its width as
$\Gamma_{Y}=(32.4\pm21.0\pm1.8)~\rm{MeV}$.
