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(1)

Image Processing

Fourier Transform

(2)

Function Spaces

Images are not vectors. Images are mappings:

Moreover, images are functions (continuous domain):

However, functions can be seen as vectors as well:

→ Images are not vectors, they are more, but they are vectors too

Vector Function

Domain Mapping Space

Scalar product Length

(3)

Base in vector spaces

Task: decompose a vector into its “components” in a base

with the base vectors and coefficients Properties of base vectors:

1. Vectors should span the space → decomposition exists for all 2. Vectors should be independent (no vector can be represented

as a linear combination of ) → decomposition is unique Special case – orthonormal base:

• All are orthogonal to each other, i.e. for all

(4)

Base in function spaces

The space has infinite dimension →

• Infinite number of base functions , i.e. , replaces

• A continuous function

The task is to decompose a given function into the base ones:

Orthonormal base means:

• orthogonal

• normalized

Then

(5)

Fourier Series

Space:

all periodic functions with the period , i.e.

Base functions: and Properties:

1. Orthonormal

2. Span the function space (Jean Baptiste Joseph Fourier, 1822)

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Fourier Series

Decomposition:

with

(7)

Fourier Series

(8)

Complex numbers

Euler’s Formula:

Decomposition:

Coefficients:

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General functions

Arbitrary periodic functions – transition Arbitrary non-periodic functions – limit 1. Coefficients become continuous

2. The sequence becomes a complex function of a real- valued argument

The summands are “not interesting” by themselves, but rather:

amplitude-spectrum and

phase-spectrum

(10)

2D Discrete Fourier Transform

Two primary arguments: and

Two frequencies: horizontal and vertical Transform:

Inverse:

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2D Discrete Fourier Transform

(12)

Amplitude-spectrums

Images

Fourier Transforms

(13)

Amplitude vs. Phase

(14)

Example – Directions

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Example – Directions

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: operator (Fourier Transform)

: the image of a function in the frequency space

Proof: … analogously

Convolution Theorem

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Convolution Theorem

Corollary 1:

a convolution can be performed in the frequency space by

Time complexity:

Fourier Transform can be done with

Component-by-component multiplication:

→ all together

instead of by the direct implementation Corollary 2:

each filter has its spectral characteristics in the frequency space.

(18)

Convolution Theorem

Some filters and their spectrums

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Further themes:

Image say “where” but not “what”.

Spectrums say “what” but not “where”.

Windowed Fourier Transform – spectrums for (small) windows at each position.

Cosine Transform (1D, discrete, DCT-II – JPEG):

Wavelet Transform:

Referenzen

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