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Figure 1
A 2D representation of reciprocal space, showing RLPs of a crystal and the Ewald sphere for monochromatic diffraction. [{\bf k}_{0}] is the wavevector of the incident beam, [{\bf k}] is the outgoing wavevector elastically scattered from the structure in the object with spatial frequency [{\bf q}]. The diffraction intensity measured by a detector in the direction of vector [{\bf k}] corresponds to the intensity at the green RLP.

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