Solving James' Confusion: Abbe Theory, Spatial Filtering & Optical Computers

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SUMMARY

The discussion centers on James' confusion regarding the application of Abbe theory in optical computing, specifically in the context of spatial filtering and Fourier transforms. The setup involves a laser focused on a 10 μm screen, utilizing a series of lenses to convert wavefronts and perform low pass filtering in the Fourier plane. The phenomenon where passing vertical maxima results in horizontal lines, and vice versa, is attributed to the properties of Fourier transforms, which relate spatial frequencies to image characteristics. Understanding this relationship is crucial for grasping the underlying physics of optical filtering.

PREREQUISITES
  • Abbe theory in optics
  • Fourier transforms and their applications
  • Spatial filtering techniques
  • Optical computing fundamentals
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  • Study the principles of Fourier optics
  • Explore the effects of spatial filters on diffraction patterns
  • Learn about the mathematical formulation of Fourier transforms
  • Investigate practical applications of optical computers in image processing
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Optical engineers, physicists, and students studying optics who seek to deepen their understanding of spatial filtering and the application of Fourier transforms in optical systems.

JamesJames
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I am confused by this Abbe theory thing involvign the use of an optical computer.

A laser is focused onto a 10 μm screen with adjustable micrometer screws. A pinhole is provided to avoid any unnecessary dispersion of the laser beam. The first lens converts spherical wavefronts into plane waves which then pass through an object plane (Ronchi rulings). It could be thought of as a condenser that produces a parallel uniformly illuminated beam. The purpose of the second lens is to form the Fourier transform image in its focus (transform plane). Low pass filtering in the Fourier plane is acheived by making use of an aperture. The third lens, when placed at its focal distance from the Fourier plane, converts the Fourier image into the inverted image of the object.

Upon inserting a fine wire mesh into the object plane, a faithful representation of the image is obtained. A 2D periodic object like this generates a T shaped diffraction pattern with a high degree of symmetry.

Now here' s what is really bugging me...There are masks that pass only parts of the pattern. For example, the effect on the image of passing only the vertical principal maxima is horizontal lines using a narrow vertical slit at the plane of the T shapped diffraction pattern. Turning the slit to select only the horizontal maxima yields vertical lines.

What is going on here physically? I am confused about how passing vertical maxima yields a the ("opposite") horizontal lines and vice versa.
I' ve read up on Fourier transforms but don' t understand how this is happening.

James
 
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Anyone? I' m sure someone can help me.
 

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