Название: EEG Signal Processing and Machine Learning
Автор: Saeid Sanei
Издательство: John Wiley & Sons Limited
Жанр: Программы
isbn: 9781119386933
isbn:
The denominator is reduced if we choose:
(4.57)
This corresponds to the case where the wavelet is the difference between the squares of two resolutions:
(4.58)
The reconstruction algorithm then carries out the following steps:
1 Compute the fast Fourier transform (FFT) of the signal at the low resolution.
2 Set j to np (number of WT resolutions); perform the following iteration steps:
3 Compute the FFT of the wavelet coefficients at the scale j.
4 Multiply the wavelet coefficients Wj by .
5 Multiply the signal coefficients at the lower resolution Cj by .
6 The inverse Fourier transform of gives the coefficients Cj‐1.
7 j = j − 1 and return to step 3.
The use of a band‐limited scaling function allows a reduction of sampling at each scale and limits the computation complexity.
The WT has been widely used in EEG signal analysis. Its application to seizure detection, especially for neonates, modelling of the neuron potentials, and the detection of EP and ERPs will be discussed in the corresponding chapters of this book.
4.5.2 Synchro‐Squeezed Wavelet Transform
The synchro‐squeezing wavelet transform (SSWT) has been introduced as a post‐processing technique to enhance the TF spectrum obtained by applying the WT [23]. Assuming that the input f(t) is a pure harmonic signal (f(t) = Acos(ωt)), using Plancherel's theorem, the following equations are derived from (4.20) [23]:
One assumption in the above equation (Eq. 4.59) is that the selected mother wavelet is concentrated within the positive energy range, which means
(4.60)
Considering the selected pure harmonic signal f(t) = Acos(ωt), it is simple to observe that ω(a, b) = ω. The candidate IFs are exploited to recover the actual frequencies. Therefore, a reallocation technique has been used to map the time domain into TF domain using (b, a) ⇒ (b, ω(a, b)). Based on this, each value of W(a, b) (computed at discrete values of ak ) is re‐allocated into Tf (ωl , b) as provided in the following equation (Eq. 4.61):
where ωl is the nearest frequency to the original point ω(a, b), ∆ω is the width of the frequency bins
4.5.3 Ambiguity Function and the Wigner–Ville Distribution
The ambiguity function for a continuous time signal is defined as:
(4.62)
This function has its maximum value at the origin as
(4.63)
As an example, if we consider a continuous time signal consisting of two modulated signals with different carrier frequencies such as
(4.64)
The ambiguity function Ax (τ,ν) will be in the form of:
(4.65)
This concept is very important in separation of signals using the TF domain. This will be addressed in the context of blind source separation (BSS) later in this chapter. Figure 4.8 demonstrates this concept.
The Wigner–Ville frequency distribution of a signal x(t) is then defined as the two‐dimensional Fourier transform of the ambiguity function:
(4.66)
which changes to the dual form of the ambiguity СКАЧАТЬ