Varying thickness diffraction grating

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SUMMARY

The discussion centers on the behavior of plane waves passing through a diffraction grating with varying thickness, explaining how this results in the formation of multiple plane waves at different angles. The Huygens-Fresnel principle is referenced to illustrate how a plane wave transforms into a spherical wave. The conversation emphasizes that the phase variations caused by the thickness differences lead to constructive interference, enhancing the diffraction pattern. It is noted that the depth of the thickness variations must be precise, ideally a fraction of a wavelength, to optimize the effect.

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  • Understanding of the Huygens-Fresnel principle
  • Knowledge of diffraction and interference patterns
  • Familiarity with the concept of Young's Slits
  • Basic principles of optical physics
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  • Study the mathematical formulation of diffraction grating
  • Explore the effects of varying thickness on optical path length
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DariusP
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I know that a plane wave going through a slit becomes a spherical wave because of a Huygens-Fresnel principle. Can someone explain to me why a plane wave splits into many plane waves with different directions when going through a plate with varying thickness?
upload_2019-1-7_11-5-51.png


Can someone explain me this image?
 

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It's a picture of a diffraction grating. The maxima are in the directions where the contributions from each of the strips on the plate are in phase. It works for opaque strips, as with a conventional diffraction grating and for any other periodic variation across the aperture.
Look up Young's Slits for the basic way that a diffraction / interference pattern is formed and then look up Diffraction Grating, which is basically no more than multiple Young's Slits. A normal diffraction grating blocks at least half of the incident light and what's left will form the diffraction pattern. Using periodic thickness variations will produce phase variations of contributions from all parts of the surface through. Instead of just blocking half of the light, the variations in thickness phase over different paths allow constructive interference from all over the surface.
That diagram is really not very good at demonstrating the effect and it doesn't make clear that the 'lenses' need to be the right depth for it to work best. It would require the path lengths through the lenses to give an appropriate phase variation over each element - perhaps in the order of a fraction of a wavelength (?) i.e. very shallow thickness variations.
 
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