Pendellösung
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The Pendellösung effect or phenomenon is seen in diffraction in which there is a
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in the intensity of electromagnetic waves travelling within a crystal lattice. It was predicted by P. P. Ewald in 1916 and first observed in electron diffraction of
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in 1942. At the exit surface of a
photonic crystal A photonic crystal is an optical nanostructure in which the refractive index changes periodically. This affects the propagation of light in the same way that the structure of natural crystals gives rise to X-ray diffraction and that the atomic ...
(PhC), the intensity of the diffracted wave can be periodically modulated, showing a maximum in the "positive" (forward diffracted) or in the "negative" (diffracted) direction, depending on the crystal slab thickness. The Pendellösung effect in
photonic crystal A photonic crystal is an optical nanostructure in which the refractive index changes periodically. This affects the propagation of light in the same way that the structure of natural crystals gives rise to X-ray diffraction and that the atomic ...
s can be understood as a beating phenomenon due to the phase modulation between coexisting plane wave components, propagating in the same direction. This thickness dependence is a direct result of the so-called Pendellösung phenomenon, consisting of the periodic exchange inside the crystal of the energy between direct and diffracted beams. The Pendellösung interference effect was predicted by dynamical diffraction and also by its fellow theories developed for visible light.


References

Condensed matter physics Metamaterials Photonics {{CMP-stub