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Figure 4
Variation of symmetry-adapted atomic displacements, |d|, with respect to the parent cubic structure, derived from original data of Senn et al. (2015BB46) refined in space group Cc. Three different crystals, c8 (red), c11 (blue), c17 (green), were from the same original batch as used for determination of the temperature dependence of lattice parameters shown in Fig. S10a. (a) Temperature dependence of average values of displacements with symmetry [{{\Gamma}}_5^ +, ] Δ5, X1, X3, W1 and W2. (b) Comparison of the average displacement amplitude |dΓ5+| with variations of e4 and e6, showing that it has the same temperature dependence as the average value of shear strains belonging to irrep [{{\Gamma}}_5^ +]. (c) Temperature dependence of values of individual displacement modes with symmetry [{{\Gamma}}_5^ +, ] Δ5, X1, X3, W1 and W2. [\left| {{d_{6{{\Delta}}5}}} \right|] is mode 37 in the list of modes from Senn et al. (2015BB46), [\left| {{d_{6{\rm X}1}}} \right|] is mode 43, [\left| {{d_{5{\rm X}3}}} \right|] is mode 78, [\left| {{d_{3{\rm W}1}}} \right|] is mode 61, [\left| {{d_{6{\rm W}2}}} \right|] is mode 68. (d) Variations of average |d| values for different symmetries with respect to variation of |dΔ5|: all are approximately linear but straight lines through the data do not pass through the origin. (e) Comparison of individual |d| variations selected as displaying the largest temperature dependences for different symmetries with the variation of the individual values [\left| {{d_{6{{\Delta}}5}}} \right|]: straight lines through the data were constrained to pass through the origin showing that the X1, W1 and X3 modes can be understood as scaling linearly with the Δ5 mode. (f) A straight line through data, constrained to pass through zero, shows that the W2 mode can be understood as scaling with the square of the Δ5 mode.

Journal logo STRUCTURAL SCIENCE
CRYSTAL ENGINEERING
MATERIALS
ISSN: 2052-5206
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