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Figure 4
The angular dependence as a function of time of the centre of mass of the main diffraction peak expressed in the angle with respect to the original position of the sample after a rotation of the sample to 45°. The interaction with the magnetic fields is the reason for the rotation back to the original position. It is interesting that at some temperatures it is clear that this is not a homogeneous rotation since the data indicate a counter rotation.

Journal logoJOURNAL OF
APPLIED
CRYSTALLOGRAPHY
ISSN: 1600-5767
Volume 40| Part s1| January 2007| Pages s52-s56
doi:10.1107/S0021889806054823
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