Amplitudes of $\mathrm{GM}_{4}^{+}$(spheres), $\mathrm{X}_{3}^{+}$(stars), the global amplitude-value for the tri-dimensional $\mathrm{X}_{5}^{+}$irreps (squares) and its components: A10 (circles), A11 (up triangle) and A11 (down triangle), in the room-temperature structures of the $\mathrm{Ln}_{2} \mathrm{CoMnO}_{6}\left(\mathrm{Ln}=\mathrm{La}[\mathrm{PW}], \mathrm{La}^{* 115}, \mathrm{La}^{* * 119}, \mathrm{Lu}^{128} \mathrm{Nd}^{* 129}, \mathrm{Nd}^{* * 130}\right)$, $\mathrm{Ln}_{2} \mathrm{NiMnO}_{6}\left(\mathrm{Ln}=\mathrm{La} \sqrt{115}, \mathrm{La}^{* * *} \sqrt{134}, \mathrm{ Tb} \sqrt{118}, \mathrm{Sm}{ }^{\underline{118}}, \mathrm{Sm}^{*} \sqrt{135}, \mathrm{Hc} \xrightarrow{131}\right), \mathrm{Y}_{2} \mathrm{NiMnO}_{6} \sqrt{132}$ and $\mathrm{Bi}_{2} \mathrm{NiMnO}_{6} \sqrt{133}$ compounds, versus the tolerance factor values, calculated using bond distances. PW stands for present work: $[\mathrm{PW}]$ with all modes freed and $\left[\mathrm{PW}^{*}\right]$ only the effectively acting ones, see text.
Amplitudes of \mathrm{GM}_{4}^{+}(spheres), \mathrm{X}_{3}^{+}(stars), the global amplitude-value for the tri-dimensional \mathrm{X}_{5}^{+}irreps (squares) and its components: A10 (circles), A11 (up triangle) and A11 (down triangle), in the room-temperature structures of the \mathrm{Ln}_{2} \mathrm{CoMnO}_{6}\left(\mathrm{Ln}=\mathrm{La}[\mathrm{PW}], \mathrm{La}^{* 115}, \mathrm{La}^{* * 119}, \mathrm{Lu}^{128} \mathrm{Nd}^{* 129}, \mathrm{Nd}^{* * 130}\right), \mathrm{Ln}_{2} \mathrm{NiMnO}_{6}\left(\mathrm{Ln}=\mathrm{La} \sqrt{115}, \mathrm{La}^{* * *} \sqrt{134}, \mathrm{ Tb} \sqrt{118}, \mathrm{Sm}{ }^{\underline{118}}, \mathrm{Sm}^{*} \sqrt{135}, \mathrm{Hc} \xrightarrow{131}\right), \mathrm{Y}_{2} \mathrm{NiMnO}_{6} \sqrt{132} and \mathrm{Bi}_{2} \mathrm{NiMnO}_{6} \sqrt{133} compounds, versus the tolerance factor values, calculated using bond distances. PW stands for present work: [\mathrm{PW}] with all modes freed and \left[\mathrm{PW}^{*}\right] only the effectively acting ones, see text.