Pole Figures
Documentation for this module will be added soon.
Map every point on the fiber by all crystal symmetries and keep the one closest to identity.
Sweep the point around the Bragg circle to visualize the full surface of orientations contributing to this reflection.
Integrate the ODF along each fiber and project intensities onto a flat detector.
For a crystal with lattice planes (hkl) and d-spacing d, Bragg’s law 2d sinθ = λ determines the scattering angle. With the beam along x, the plane normal must lie on a cone at angle 90°−θB from the beam — the blue circle on S². Each point on that circle defines a scattering direction; the set of crystal orientations producing that diffraction spot forms a fiber in orientation space, shown as a yellow curve in Rodrigues representation.