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Figure 3
For all 2D systems except the oblique case, which has no generic solution, two homophase layers share the same crystallographic row defined by the lattice node [z = n+m\rho \exp({i\varphi})], with n and m coprimes, if there exists an equivalent lattice node [z^{\prime} = \bar{z}\exp({2i\theta})] deduced from z by a mirror in the direction θ defined by: rectangle [\theta = 0,\pi/2], square [\theta = 0,\pi/4] and hexagon [\theta = 0,\pi/6].

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