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Crystal lattices
Burzlaff, H., Grimmer, H., Gruber, B., Wolff, P. M. de and Zimmermann, H.  International Tables for Crystallography (2016). Vol. A, ch. 3.1, pp. 698-719 [ doi:10.1107/97809553602060000929 ]
... last two sections of the chapter. 3.1.1. Bases and lattices H. Burzlaff a andH. Zimmermann e 3.1.1.1. Description and transformation of ... Two dimensions. Lattice point group22mm4mm6mm Crystal family† m o t h monoclinic (oblique) orthorhombic (rectangular) tetragonal (square) hexagonal (b) Three dimensions. Lattice point group Crystal family† a m o t h c anorthic (triclinic) monoclinic orthorhombic tetragonal hexagonal cubic †The ...

Conventional characters
Gruber, B. and Grimmer, H.  International Tables for Crystallography (2016). Vol. A, Section 3.1.4.5, pp. 717-718 [ doi:10.1107/97809553602060000929 ]
Conventional characters 3.1.4.5. Conventional characters Lattice characters were defined in Section 3.1.4.2 by dividing the Niggli image of a certain Bravais type into components. Doing the same - instead of with the Niggli points - with the parameters of conventional cells7 of lattices of the Bravais type we obtain a division of the ...
     [more results from section 3.1.4 in volume A]

Magnetic properties
Borovik-Romanov, A. S., Grimmer, H. and Kenzelmann, M.  International Tables for Crystallography (2013). Vol. D, ch. 1.5, pp. 106-153 [ doi:10.1107/97809553602060000904 ]
... given by This equation shows how the units of B, H and M are related in the Gaussian system. The unit for B, the gauss (G), and for H, the oersted (Oe), also coincide in magnitude, whereas the unit ... that is valid in both systems. Historically, the two fields H and B have been called the magnetic field H ...

Connection between Gaussian and SI units
Borovik-Romanov, A. S., Grimmer, H. and Kenzelmann, M.  International Tables for Crystallography (2013). Vol. D, Section 1.5.10, p. 148 [ doi:10.1107/97809553602060000904 ]
Connection between Gaussian and SI units 1.5.10. Connection between Gaussian and SI units Numerical values of magnetic quantities are given in the tables and figures in this chapter in Gaussian units together with information on how the corresponding values in SI units are obtained. As a summary, Table 1.5.10.1 gives for ...

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 ...
     [more results from section 1.5.9 in volume D]

Multiferroics
Borovik-Romanov, A. S., Grimmer, H. and Kenzelmann, M.  International Tables for Crystallography (2013). Vol. D, Section 1.5.8.3, pp. 143-145 [ doi:10.1107/97809553602060000904 ]
... polarization induced along [001] was measured. If the applied field H was increased beyond 6kOe (B = 6kG = 0.6T), the induced polarization ... weakly ferromagnetic Ni3B7O13I at 46K (Ascher et al., 1966). H = 1kOe corresponds to B = 1kG = 0.1T. If the spontaneous polarization ... representations, [Gamma]2 and [Gamma]3. Since the coupling term H has to be invariant under all symmetry elements of ...
     [more results from section 1.5.8 in volume D]

Linear magnetic birefringence
Borovik-Romanov, A. S., Grimmer, H. and Kenzelmann, M.  International Tables for Crystallography (2013). Vol. D, Section 1.5.7.3, pp. 138-139 [ doi:10.1107/97809553602060000904 ]
... magnetic crystals. Rep. Prog. Phys. 47, 513-611. Le Gall, H., Leycuras, C., Minella, D., Rudashevskii, E. G. & Merkulov, V. S. ... 1223-1225. Merkulov, V. S., Rudashevskii, E. G., Le Gall, H. & Leycuras, C. (1981). Linear magnetic birefringence of hematite in ...
     [more results from section 1.5.7 in volume D]

Reorientation transitions
Borovik-Romanov, A. S., Grimmer, H. and Kenzelmann, M.  International Tables for Crystallography (2013). Vol. D, Section 1.5.6, pp. 132-133 [ doi:10.1107/97809553602060000904 ]
... point group is = . Let us apply the magnetic field H parallel to the twofold axis x (see Fig. 1.5.6.2). ...

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 ...
     [more results from section 1.5.5 in volume D]

Ferroic domains
Borovik-Romanov, A. S., Grimmer, H. and Kenzelmann, M.  International Tables for Crystallography (2013). Vol. D, Section 1.5.4.3, p. 128 [ doi:10.1107/97809553602060000904 ]
... ferroic crystals. Eur. Phys. J. B, 71, 315-320. Schmid, H. (2008). Some symmetry aspects of ferroics and single phase ...
     [more results from section 1.5.4 in volume D]

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