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 Results for DC.creator="H." AND DC.creator="Grimmer" in section 1.5.9 of volume D
The difference between the magnetic anisotropies at zero strain and zero stress
Borovik-Romanov, A. S., Grimmer, H. and Kenzelmann, M.  International Tables for Crystallography (2013). Vol. D, Section 1.5.9.3, p. 148 [ doi:10.1107/97809553602060000904 ]
The difference between the magnetic anisotropies at zero strain and zero stress 1.5.9.3. The difference between the magnetic anisotropies at zero strain and zero stress The spontaneous magnetostriction makes a contribution to the magnetic anisotropy (especially in crystals with a cubic prototype). Therefore, to find the full expression for the ...

Magnetostriction in an external magnetic field
Borovik-Romanov, A. S., Grimmer, H. and Kenzelmann, M.  International Tables for Crystallography (2013). Vol. D, Section 1.5.9.2, pp. 147-148 [ doi:10.1107/97809553602060000904 ]
Magnetostriction in an external magnetic field 1.5.9.2. Magnetostriction in an external magnetic field There are three reasons for the magnetostriction arising in a magnetic field: (a) the transfer of the crystal into a single-domain state if the magnetic field is directed along one of the easy axes; (b) the deflection ...

Spontaneous magnetostriction
Borovik-Romanov, A. S., Grimmer, H. and Kenzelmann, M.  International Tables for Crystallography (2013). Vol. D, Section 1.5.9.1, pp. 145-147 [ doi:10.1107/97809553602060000904 ]
Spontaneous magnetostriction 1.5.9.1. Spontaneous magnetostriction In this section, we shall assume that the crystal under consideration undergoes a phase transition from the paramagnetic state into a magnetically ordered state. The latter is a single-domain state with the magnetization (or the antiferromagnetic vector) aligned along the vector . As was mentioned ...

Magnetostriction
Borovik-Romanov, A. S., Grimmer, H. and Kenzelmann, M.  International Tables for Crystallography (2013). Vol. D, Section 1.5.9, pp. 145-148 [ doi:10.1107/97809553602060000904 ]
Magnetostriction 1.5.9. Magnetostriction The transition to an ordered magnetic state is accompanied by a spontaneous distortion of the lattice, which is denoted spontaneous magnetostriction. The lattice distortion may be specified by the deformation (strain) components . The undeformed state is defined as the crystal structure that would be realized if the ...

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