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 Results for DC.creator="A." AND DC.creator="S." AND DC.creator="Borovik-Romanov" in section 1.5.5 of volume D
Other weakly non-collinear magnetic structures
Borovik-Romanov, A. S., Grimmer, H. and Kenzelmann, M.  International Tables for Crystallography (2013). Vol. D, Section 1.5.5.2, p. 132 [ doi:10.1107/97809553602060000904 ]
... collinear magnetic structures 1.5.5.2. Other weakly non-collinear magnetic structures A thermodynamic potential of the form (1.5.5.1) may give rise not ... to the reverse phenomenon. If the coefficient B (instead of A) changes its sign and , the material will undergo a transition into a slightly canted ferromagnetic structure, in which ...

Weak ferromagnetism
Borovik-Romanov, A. S., Grimmer, H. and Kenzelmann, M.  International Tables for Crystallography (2013). Vol. D, Section 1.5.5.1, pp. 128-132 [ doi:10.1107/97809553602060000904 ]
... material () and the thermodynamic potential of the material contains such a term, the minimum of the potential will be obtained only if as well. The term is a relativistic one. Therefore this effect must be small. We shall ... crystals was derived in Section 1.5.3.3. For the case of a two-sublattice antiferromagnet, one has to add to the ...

Weakly non-collinear magnetic structures
Borovik-Romanov, A. S., Grimmer, H. and Kenzelmann, M.  International Tables for Crystallography (2013). Vol. D, Section 1.5.5, pp. 128-132 [ doi:10.1107/97809553602060000904 ]
... of magnetic ordering. Some magnetic structures can be described as a superposition of two antiferromagnetic structures with perpendicular antiferromagnetic vectors . ... be called weakly non-collinear antiferromagnets. There can also be a superposition of an antiferromagnetic structure with a ferromagnetic one (with ). This phenomenon is called weak ...

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