Difference between Bragg and Laue Diffraction?

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Bragg and Laue diffraction both describe elastic scattering from a periodic lattice but differ in their assumptions. Bragg diffraction focuses on specific families of planes and requires specular reflection, while Laue diffraction does not impose these restrictions and relies on the concept of a reciprocal lattice. The Laue condition is more general, allowing for various planes and directions of scattering. The distinction regarding specular reflection in Bragg diffraction is often a simplification, as multiple lattice planes can produce reflections in various directions. Understanding these differences is crucial for applying each method effectively in crystallography.
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Hi! I am confused about the difference between the Bragg and Laue Diffraction. It seems that both arrive at the same result, but the assumptions for both are different?
 
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What are the differences in assumptions? I can't think of any. They both deal with elastic scattering off a periodic lattice.
 
The Bragg condition considers lattice objects that are grouped in families of planes, and the incident radiation is specularly reflected. The Laue condition doesn't require the assumption of particular planes and spacings, and doesn't require that reflection be specular.
 
The Laue criterion is dependent upon the construction of a reciprocal lattice. That requires the existence of the direct lattice (consisting of families of planes defined by Miller Indices), upon which the Bragg condition is derived.

The apparent difference regarding specular reflection is an artifact of the way in which Bragg reflection is commonly depicted - by looking at only one family of planes. In reality, through every point in the real lattice, one can construct a virtually infinite number of lattice planes, each of which produces a specular reflection in a different direction.
 
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I am observing an irregular, aperiodic noise pattern in the reflection signal of a high-finesse optical cavity (finesse ≈ 20,000). The cavity is normally operated using a standard Pound–Drever–Hall (PDH) locking configuration, where an EOM provides phase modulation. The signals shown in the attached figures were recorded with the modulation turned off. Under these conditions, when scanning the laser frequency across a cavity resonance, I expected to observe a simple reflection dip. Instead...

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