SIGNAL PROCESSING OF RADAR ECHOES USING WAVELETS AND HILBERT HUANG TRANSFORM
Wavelets Applications in Signal and Image Processing.
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Transcript of Wavelets Applications in Signal and Image Processing.
Wavelets
Applications in Signal and Image Processing
The Fourier Transform
Motivation!
Problem
The FT of stationary and non stationary signals with the same frequency components are equivalent.
i.e. we are lacking time localization
Although FT tells us what frequencies appear in the signal it does not tell us at what time they appear!
What has caused this?
e-2iπf is a function of infinite support / infinite window function
Short Term Fourier Transform: STFT
Multiple FT over smaller windows translated in time
Compactly supported
We now have a time-frequency representation
YOU CAN ALL GO HOME
NOT!
Recall: In the time domain we know exactly the value of the
signal at any time (time resolution) In the frequency domain we know exactly the frequencies
in the signal (frequency resolution)
In STFT the kernel is compact … thus we can only see a band of frequencies based on the size of the kernel
Consequence
Window size is application specific
Narrow window -> good time resolution, poor frequency resolution
Wide window -> good frequency resolution, poor time resolution
Increasing window width
Wavelets to the rescue
We would like to develop a method independent of the windowing function that gives usa) Good time resolution and poor frequency resolution at
high frequencies
b) Good frequency resolution but poor time resolution at low frequencies
Low frequency => Signal information
High frequency => Excess detail or noise in the signal
Continuous Wavelet Transform: CWT
Ψ is the mother wavelet, the shape or choice of this depend on the properties of the signal we wish to analyze
Time localization
Inspect the signal at different time steps
Introduce a translation parameter, t’, that controls the translation of the function:
Frequency Localization
Inspect the signal for different frequencies
Introduce a dilation parameter, s, that controls the scale of the function:
Result
Changing translation parameter: Time Localization
Changing dilation
parameter: Frequency
Localization
Result
+ve response
-ve response
0 response
Low response
Orthogonality / Orthonormal
Orthogonal: i.e. 2 functions are, at no place the same or, are
symmetric
Orthonormal: So dilations and translations of a wavelet must be
orthonormal to itself so as not to influence the construction of the coefficients
These allow for perfect reconstructions of the form
Inverse Wavelet Transform: ICWT
Denoise by zeroing out coefficients
Frequency to time resolution
STFT has constant time to frequency resolution as window size is fixed
Low scales / high frequencies have
good time resolution but poor frequency
resolution.
High scales / low frequencies have good frequency
resolution but poor time resolution.
Discrete Wavelet Transform: DWT
The Discrete Wavelet Transform is a sampled version of the Continuous case with discrete dilation and translation parameters
Filters or different cut of frequencies are used to analyze the signal at different scales or resolutions
We will be requiring a scaling filter/function and a wavelet filter/function in this case Scaling function – low pass filter - approximation Wavelet – high pass filter - details
Discrete wavelet Ψ
Recall that the CW is defined as:
In a continuous transform we find the inner product over all scales S and translates t’. However now we must sample s and t’.
Logarithmic sampling of s means we need to move in discrete steps on t’ proportional to the scale s.
Dyadic scaling
Dyadic scaling, choose s0=2 and t0’=1
Later this will lead to a nice down sampling routine
DWT to obtain detail coefficients becomes:
Dyadic scaling
Discrete scaling function Φ
In the CWT we calculated the set of coefficients ψ over all scales s and translations t’ on the continuous signal x(t)
As we are sampling x(t) we cannot have these infinite coefficients. We need some way of keeping track of what the wavelet coefficients don’t express.
Therefore we must define how we sample the signal based on the current dilation, m, of the wavelet. This is done via a Scaling function
We can convolve the signal with the scaling function to get approximation coefficients
Discrete scaling function Φ
Approximation and detail
Approximation coefficients, ϕ, are produced by applying the scaling function to the sampled signal. They express the signal at a lower resolution as if the high frequencies had been removed
Detail coefficients, ψ, are produced by applying the wavelet to the sampled signal. They express the higher frequency components in the signal.
Thus a signal is represented as the sum of approximation and detail coefficients:
Multi-Resolution Analysis, MRA
Haar example
DWT via Filtering
Filter convolution :
H (equivalent to wavelet) is high pass, stripping the signal of its lower band frequencies thus its coefficients represent high frequency components
G (equivalent to scaling function) is a low pass, stripping the signal of its higher frequencies thus is passed on to the next scale to remove the next band of high frequency
DWT via Lifting
Filters can be transformed in the time or frequency domain into distinct in-place processing steps on the signal rather than costly convolutions
Expressing a wavelet in terms of lifting steps is know as a Second Generation Wavelet
Here rather than low and high pass filters we perform a Prediction step and an Update step Prediction – high pass filter – we predict what the signal is Update – low pass filter – based on the prediction we
update the signal
Lifting
Haar Lifting example Take signal x(t) and split it into odd and even pairs
As a prediction step take the odd away from the even: dj-1= oddj-P(evenj)
As an update step take the mean value of the odd and even parts Sj-1=evenj+U(dj-1)
2D DWT
Wavelets and scaling functions are orthogonal … hence separable.
We can apply the transform in one direction then the other
Z-transform
Fourier Series:
Z-Transform:
Convolution Shift Left Shift Right Down sample Up sample
Lifting to Polyphase
Split:
Prediction:
Update:
Filters to Z-transform
Lifting to Filters
Filter Results = Polyphase Lifting
Further reading
Boundary problems!
Vanishing Moments!
Wavelet packets
Second generation wavelets
Multiwavelets
Curvelets, ridgelets …
Any Questions?