Linear Filtering – Part II

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Linear Filtering – Part II Selim Aksoy Department of Computer Engineering Bilkent University
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Linear Filtering – Part II Selim Aksoy Department of Computer Engineering Bilkent University saksoy@cs.bilkent.edu.tr

Fourier theory The Fourier theory shows how most real functions can be represented in terms of a basis of sinusoids. The building block: A sin( ωx + Φ ) Add enough of them to get any signal you want. Adapted from Alexei Efros, CMU CS 484, Fall 2015 ©2015, Selim Aksoy

Fourier transform CS 484, Fall 2015 ©2015, Selim Aksoy

Fourier transform CS 484, Fall 2015 ©2015, Selim Aksoy

Fourier transform CS 484, Fall 2015 ©2015, Selim Aksoy

Fourier transform CS 484, Fall 2015 ©2015, Selim Aksoy

Fourier transform CS 484, Fall 2015 ©2015, Selim Aksoy

Fourier transform CS 484, Fall 2015 ©2015, Selim Aksoy

Fourier transform To get some sense of what basis elements look like, we plot a basis element --- or rather, its real part --- as a function of x,y for some fixed u, v. We get a function that is constant when (ux+vy) is constant. The magnitude of the vector (u, v) gives a frequency, and its direction gives an orientation. The function is a sinusoid with this frequency along the direction, and constant perpendicular to the direction. u v Adapted from Antonio Torralba CS 484, Fall 2015 ©2015, Selim Aksoy

Fourier transform Here u and v are larger than in the previous slide. Adapted from Antonio Torralba CS 484, Fall 2015 ©2015, Selim Aksoy

Fourier transform And larger still... v u Adapted from Antonio Torralba CS 484, Fall 2015 ©2015, Selim Aksoy

Fourier transform Adapted from Alexei Efros, CMU CS 484, Fall 2015 ©2015, Selim Aksoy

Fourier transform Adapted from Gonzales and Woods CS 484, Fall 2015 ©2015, Selim Aksoy

Fourier transform Adapted from Gonzales and Woods CS 484, Fall 2015 ©2015, Selim Aksoy

Fourier transform CS 484, Fall 2015 ©2015, Selim Aksoy

Fourier transform CS 484, Fall 2015 ©2015, Selim Aksoy

Fourier transform How to interpret a Fourier spectrum: fmax Horizontal orientation Vertical orientation 45 deg. fmax fx in cycles/image Low spatial frequencies High spatial frequencies Log power spectrum Adapted from Antonio Torralba CS 484, Fall 2015 ©2015, Selim Aksoy

Fourier transform C A B 1 2 3 Adapted from Antonio Torralba CS 484, Fall 2015 ©2015, Selim Aksoy

Fourier transform Adapted from Shapiro and Stockman CS 484, Fall 2015 ©2015, Selim Aksoy

Convolution theorem CS 484, Fall 2015 ©2015, Selim Aksoy

Frequency domain filtering Adapted from Shapiro and Stockman, and Gonzales and Woods CS 484, Fall 2015 ©2015, Selim Aksoy

Frequency domain filtering Since the discrete Fourier transform is periodic, padding is needed in the implementation to avoid aliasing (see section 4.6 in the Gonzales-Woods book for implementation details). CS 484, Fall 2015 ©2015, Selim Aksoy

Frequency domain filtering f(x,y) h(x,y) g(x,y)   |F(u,v)| |H(u,v)| |G(u,v)|   CS 484, Fall 2015 ©2015, Selim Aksoy Adapted from Alexei Efros, CMU

Smoothing frequency domain filters CS 484, Fall 2015 ©2015, Selim Aksoy

Smoothing frequency domain filters The blurring and ringing caused by the ideal low-pass filter can be explained using the convolution theorem where the spatial representation of a filter is given below. CS 484, Fall 2015 ©2015, Selim Aksoy

Sharpening frequency domain filters CS 484, Fall 2015 ©2015, Selim Aksoy

Sharpening frequency domain filters Adapted from Gonzales and Woods CS 484, Fall 2015 ©2015, Selim Aksoy

Sharpening frequency domain filters Adapted from Gonzales and Woods CS 484, Fall 2015 ©2015, Selim Aksoy

Template matching Correlation can also be used for matching. If we want to determine whether an image f contains a particular object, we let h be that object (also called a template) and compute the correlation between f and h. If there is a match, the correlation will be maximum at the location where h finds a correspondence in f. Preprocessing such as scaling and alignment is necessary in most practical applications. CS 484, Fall 2015 ©2015, Selim Aksoy

Template matching Adapted from Gonzales and Woods CS 484, Fall 2015 ©2015, Selim Aksoy

Face detection using template matching: face templates. CS 484, Fall 2015 ©2015, Selim Aksoy

Face detection using template matching: detected faces. CS 484, Fall 2015 ©2015, Selim Aksoy

Resizing images How can we generate a half-sized version of a large image? Adapted from Steve Seitz, U of Washington CS 484, Fall 2015 ©2015, Selim Aksoy

Resizing images 1/8 1/4 Throw away every other row and column to create a 1/2 size image (also called sub-sampling). Adapted from Steve Seitz, U of Washington CS 484, Fall 2015 ©2015, Selim Aksoy

Resizing images 1/2 1/4 (2x zoom) 1/8 (4x zoom) Does this look nice? Adapted from Steve Seitz, U of Washington CS 484, Fall 2015 ©2015, Selim Aksoy

Resizing images We cannot shrink an image by simply taking every k’th pixel. Solution: smooth the image, then sub-sample. Gaussian 1/8 Gaussian 1/4 Gaussian 1/2 Adapted from Steve Seitz, U of Washington CS 484, Fall 2015 ©2015, Selim Aksoy

Resizing images Gaussian 1/2 Gaussian 1/4 (2x zoom) Adapted from Steve Seitz, U of Washington CS 484, Fall 2015 ©2015, Selim Aksoy

Sampling and aliasing Adapted from Steve Seitz, U of Washington CS 484, Fall 2015 ©2015, Selim Aksoy

Sampling and aliasing Errors appear if we do not sample properly. Common phenomenon: High spatial frequency components of the image appear as low spatial frequency components. Examples: Wagon wheels rolling the wrong way in movies. Checkerboards misrepresented in ray tracing. Striped shirts look funny on color television. CS 484, Fall 2015 ©2015, Selim Aksoy

Gaussian pyramids Adapted from Gonzales and Woods CS 484, Fall 2015 ©2015, Selim Aksoy

Gaussian pyramids Adapted from Michael Black, Brown University CS 484, Fall 2015 ©2015, Selim Aksoy

Gaussian pyramids Adapted from Michael Black, Brown University CS 484, Fall 2015 ©2015, Selim Aksoy