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Figure 7
The emergence of an `assemblage' of `integrant points' according to Bravais. The `rows' OAA′A′′…, ABB′B′′…, with `parameter' OA first constitute a plane `lattice'. A stacking of such `lattices' following ODD′D′′… produces the `assemblage' which models the crystal (Bravais, 1848BB3).

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