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Convolution Fourier Convolution

Convolution Fourier Convolution. Outline  Review linear imaging model  Instrument response function vs Point spread function  Convolution integrals • Fourier Convolution • Reciprocal space and the Modulation transfer function  Optical transfer function  Examples of convolutions

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Convolution Fourier Convolution

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  1. Convolution Fourier Convolution Outline Review linear imaging model  Instrument response function vs Point spread function  Convolution integrals • Fourier Convolution • Reciprocal space and the Modulation transfer function  Optical transfer function  Examples of convolutions  Fourier filtering  Deconvolution  Example from imaging lab • Optimal inverse filters and noise

  2. Instrument Response Function The Instrument Response Function is a conditional mapping, the form of the map depends on the point that is being mapped. This is often given the symbol h(r|r’). Of course we want the entire output from the whole object function, and so we need to know the IRF at all points.

  3. Space Invariance Now in addition to every point being mapped independently onto the detector, imaging that the form of the mapping does not vary over space (is independent of r0). Such a mapping is called isoplantic. For this case the instrument response function is not conditional. The Point Spread Function (PSF) is a spatially invariant approximation of the IRF.

  4. Space Invariance Since the Point Spread Function describes the same blurring over the entire sample, The image may be described as a convolution, or,

  5. Convolution Integrals Let’s look at some examples of convolution integrals, So there are four steps in calculating a convolution integral: #1. Fold h(x’) about the line x’=0 #2. Displace h(x’) by x #3. Multiply h(x-x’) * g(x’) #4. Integrate

  6. Convolution Integrals Consider the following two functions: #1. Fold h(x’) about the line x’=0 #2. Displace h(x’) by x x

  7. Convolution Integrals

  8. Convolution Integrals Consider the following two functions:

  9. Convolution Integrals

  10. Some Properties of the Convolution commutative: associative: multiple convolutions can be carried out in any order. distributive:

  11. Convolution Integral Recall that we defined the convolution integral as, One of the most central results of Fourier Theory is the convolution theorem (also called the Wiener-Khitchine theorem. where,

  12. Convolution Theorem In other words, convolution in real space is equivalent to multiplication in reciprocal space.

  13. Convolution Integral Example We saw previously that the convolution of two top-hat functions (with the same widths) is a triangle function. Given this, what is the Fourier transform of the triangle function? = ?

  14. Proof of the Convolution Theorem The inverse FT of f(x) is, and the FT of the shifted g(x), that is g(x’-x)

  15. Proof of the Convolution Theorem So we can rewrite the convolution integral, as, change the order of integration and extract a delta function,

  16. Proof of the Convolution Theorem or, Integration over the delta function selects out the k’=k value.

  17. Proof of the Convolution Theorem This is written as an inverse Fourier transformation. A Fourier transform of both sides yields the desired result.

  18. Fourier Convolution

  19. Reciprocal Space real space reciprocal space

  20. Filtering We can change the information content in the image by manipulating the information in reciprocal space. Weighting function in k-space.

  21. Filtering We can also emphasis the high frequency components. Weighting function in k-space.

  22. Modulation transfer function

  23. Optics with lens

  24. Optics with lens

  25. Optics with lens

  26. Optics with lens 2D FT

  27. Optics with lens Projections

  28. Optics with lens Projections

  29. Optics with pinhole

  30. 2D FT

  31. Optics with pinhole Projections

  32. Projections

  33. Deconvolution to determine MTF of Pinhole

  34. FT to determine PSF of Pinhole

  35. Filtered FT to determine PSF of Pinhole

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