Abstract
Fig. 24 and Tables 5, 6 and 7 provide for calculations and stereographic projections for hexagonal crystals over a wide range of axial ratios.† Rhombohedral lattices referring to these hexagonal axes include the three cubic lattices with the axial ratios given in Table 5. In Fig. 24 (0001) = (00.1) hexagonal or (111) rhombohedral (cubic) is the plane of projection. The four-index system is used in the diagrams to emphasize the difference between the H and R axes but only three indices are desirable for transformations and calculations of angles etc. (see §9.2). The following notes may be of help when using Fig. 24 and Tables 5, 6 and 7:
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The rhombohedral faces have poles which fall in the position shown at equal angles ρ 2 from the threefold axis.
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Half-way between any pair of these planes, e.g. (100) and (101), is located the corresponding (110). This provides the angle λ/2, which in Fig. 24 is measured along the great circle.
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The {110} poles are at an angle ρ 1 from the centre.
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It is clear that a knowledge of any one of the three angles ρ 1,ρ 2 or λ is sufficient to determine the other two and to establish the stereographic projection completely for either a rhombohedral or a hexagonal lattice.
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The angles are functions of the hexagonal axial ratio c\a and are deduced from the general formulae given below.
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© 1967 K. W. Andrews, D. J. Dyson, and S. R. Keown
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Andrews, K.W., Dyson, D.J., Keown, S.R. (1967). Hexagonal and rhombohedral systems. In: Interpretation of Electron Diffraction Patterns. Springer, Boston, MA. https://doi.org/10.1007/978-1-4899-6475-5_10
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DOI: https://doi.org/10.1007/978-1-4899-6475-5_10
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