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Neutron Scattering - JUWEL - Forschungszentrum Jülich

Neutron Scattering - JUWEL - Forschungszentrum Jülich

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HEiDi 13<br />

Fig. 7 left: tetragonal HTT phase Fig. 7 right: orthorhombic´LTO phase<br />

4.2 Twinning<br />

During the transition into the low temperature phase the CuO6 octahedrons are tilted around<br />

their [010] axis. Thus, the two axes of identical length in the HTT phase, a1 and a2, are not<br />

equal in the LTO phase anymore. Instead, the longer one becomes the new a axis, the shorter<br />

one becomes the b axis. Whether a1 or a2 becomes the new a axis depends only on the real<br />

structure of the crystal, for instance grain boundaries or point defects. Therefore, one can find<br />

two equivalent crystallographic space groups in the LTO phase:<br />

Abma (a1 � a, a2 � b) and Bmab (a1 � b, a2 � a)<br />

For the structure factors in the LTO is valid:<br />

FAbma(hkl)=FBmab(khl)

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