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Spontaneous magnetostriction in the ordered phase of NiCI2

A. S. Baryl’nikB. I. Verkin Physicotechnical Institute of Low Temperatures, Ukrainian Academy of Sciences, 310164 KharkovA. I. ProkhvatilovB. I. Verkin Physicotechnical Institute of Low Temperatures, Ukrainian Academy of Sciences, 310164 KharkovM. A. Strzhemechnyı̆B. I. Verkin Physicotechnical Institute of Low Temperatures, Ukrainian Academy of Sciences, 310164 KharkovL. D. YantsevichB. I. Verkin Physicotechnical Institute of Low Temperatures, Ukrainian Academy of Sciences, 310164 KharkovA. F. LozenkoInstitute of Physics, Ukrainian Academy of Sciences, 252028 KievP. A. TrotsenkoInstitute of Physics, Ukrainian Academy of Sciences, 252028 KievP. M. TurchakI. Franko University, 290005 L’vov
Low Temperature Physicsjournal1994en
ABI

Аннотация

Spontaneous magnetostriction is measured for the first time in the ordered phase of NiCl2 by using two independent methods (powder x-ray diffractometry and dilatometry in crossed magnetic fields). These methods differ in that the change in the lattice parameters upon a transition to the ordered polydomain state, which is effectively isotropic in the basal plane, is measured in the former case, while the change in the sample size as a result of monodomainization of the state induced by the magnetic field is measured in the latter case. In spite of a qualitative similarity (positive striction in the hexagonal plane of magnetic ordering and compression along the c-axis), the results exhibit considerable quantitative differences. The spontaneous striction determined by using the x-ray technique is uxx = uyy = (7.2±2.2) · 10−4 in the plane and uzz = − (8.7±3.3) · 10−4 along the c-axis, which is approximately an order of magnitude larger than dilatometric value (besides, dilatometrically measured striction turns out to be strongly anisotropic in the basal plane, which is quite natural).

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