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Based on $e^{+}e^{-}$ collision data collected at center-of-mass energiesfrom 2.000 to 3.080 GeV by the BESIII detector at the BEPCII collider, apartial 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$e^{+}e^{-}\to K^{*}(892)^{0}\bar{K}$ and $K^{*}_{2}(1430)^{0}\bar{K}$ to bemeasured. The Born cross sections for $e^{+}e^{-}\to K_{S}^{0}K_{L}^{0}\pi^{0}$ are consistent with previous measurements by BaBar and SND,but with substantially improved precision. The Born cross section lineshape ofthe process $e^{+}e^{-}\to K^{*}(892)^{0}\bar{K}$ is consistent with a vectormeson state around 2.2 GeV with a statistical significance of 3.2$\sigma$. ABreit-Wigner fit determines its mass as$M_Y=(2164.1\pm9.6\pm3.1)~{\rm{MeV}}/c^{2}$ and its width as$\Gamma_{Y}=(32.4\pm21.1\pm1.5)~\rm{MeV}$, where the first uncertainties arestatistical and the second ones are systematic, respectively.

Measurement of the $e^{+}e^{-} \to K_{S}^{0} K_{L}^{0} \pi^{0}$ cross sections from $\sqrt{s}=$ 2.000 to 3.080 GeV