perovskite atlas Structures, modes and phase transitions · Josu M. Igartua · UPV/EHU

Figure 4.1 · Thesis 3 · Iturbe 2012

Figure 4.1 · Thesis 3 · Iturbe 2012

status thesis-only · visibility public · id plt:thesis-03.4.1

Graph of maximal subgroups relating the F m \overline{3} m and the P 2_{1} / c space groups of room temperature \operatorname{Sr} L n M R u \mathrm{O}_{6}(L n=\mathrm{La}, \mathrm{Nd}, \mathrm{Pr}; M=\mathrm{Zn}, \mathrm{Co}, \mathrm{Mg}, \mathrm{Ni}) phases. For each space group, the irreducible representation of the distortion mode yielding this symmetry is indicated if existing. For the parent phase (red) and isotropy groups, the corresponding simulated patterns are plotted in the P 2_{1} / n non conventional monoclinic bases. The combination of distortion modes responsible for the F m \overline{3} m \rightarrow P 2_{1} / n symmetry-breaking are plotted for P 2_{1} / n (orange).

Graph of maximal subgroups relating the F m \overline{3} m and the P 2_{1} / c space groups of room temperature \operatorname{Sr} L n M R u \mathrm{O}_{6}(L n=\mathrm{La}, \mathrm{Nd}, \mathrm{Pr}; M=\mathrm{Zn}, \mathrm{Co}, \mathrm{Mg}, \mathrm{Ni}) phases. For each space group, the irreducible representation of the distortion mode yielding this symmetry is indicated if existing. For the parent phase (red) and isotropy groups, the corresponding simulated patterns are plotted in the P 2_{1} / n non conventional monoclinic bases. The combination of distortion modes responsible for the F m \overline{3} m \rightarrow P 2_{1} / n symmetry-breaking are plotted for P 2_{1} / n (orange).

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Thesis 3 · Iturbe 2012
Figure
4.1
Kind
group-subgroup-tree
Rights
own
Reproduce
not-needed

auto-cropped from the OCR Markdown crop box (stage B); materials and kind to be reviewed in Phase 1

Evidence