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 Results for DC.creator="H." AND DC.creator="Grimmer" 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 ]
Other weakly non-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 only to the weak ferromagnetism considered above but also to the reverse phenomenon. If the coefficient B (instead of A) changes its sign and , the material will ...

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 ]
... Figure 1.5.5.2 | | Dependence of magnetization and on the magnetic field H for the weak ferromagnet MnCO3 at 4.2K (Borovik-Romanov, 1959a). (H = 1kOe corresponds to B = 1kG = 0.1T; M = 100emumol-1 = 0.1Am2mol ... ferromagnetism. In Magnetism, Vol. I, edited by G. T. Rado & H. Suhl, pp. 85-125. New York: Academic Press. Néel, ...

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 ]
... Figure 1.5.5.2 | | Dependence of magnetization and on the magnetic field H for the weak ferromagnet MnCO3 at 4.2K (Borovik-Romanov, 1959a). (H = 1kOe corresponds to B = 1kG = 0.1T; M = 100emumol-1 = 0.1Am2mol ... ferromagnetism. In Magnetism, Vol. I, edited by G. T. Rado & H. Suhl, pp. 85-125. New York: Academic Press. Néel, ...

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