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In-Depth Information
As noted before, there exists a concrete relationship between each scale and an
equivalent set of Fourier frequencies, often known as pse udo f requencies [10]. For
the Morlet wavelet used this relationship is f
ω 0 + 2 + ω
0
=
, which in our case
s
(
. In this study the power spectra is
classified in six sequential frequency bands that are coarsely mapped to the scales
tabulated in Table 3.1.
ω 0 =
6); this gives a value of f
=
1
/ (
1
.
03 s
)
Table 3.1: Frequency bands - scale set mapping
Band
Frequency
Scale
Theta (
θ
)
4-8
21, 22, 23, 24
Alpha1 (
α 1 )
8-10
20
Alpha2 (
α 2 )
10-13
18, 19
Beta (
β
)
13-30
14, 15, 16, 17
Gamma1 (
γ 1 )
30-45
11, 12, 13
Gamma2 (
γ 2 )
45-90
7, 8, 9, 10
The first stage of our fe atu re extraction method is based on capturing the time-
averaged power spectrum W n 2
f or each electrode and scale, which is computed by
2
averaging the power spectrum
W n
over time:
N
1
n = 0 W n ( s )
W n 2
2
(
s
)=(
1
/
N
)
.
(3.6)
Further averaging in scale is performed, in order to map a single f eat ure per fre-
quency band of interest. Thus, the scale-averaged power spectrum W n 2
is defined
(
)
as the weighted sum of the wavelet power spectrum
over scales s j 1 to
s j 2 within each frequency band, with scale correspondences defined in Table 3.1.
Based on these definitions, the average power over time and frequency band is
obtained as
W n
s
j = j 1 W n ( s j )
j 2
s j ,
2
W s , n =( δ
j
/ δ
t
/
C δ )
/
(3.7)
where C δ is a constant scale-independent factor used for the exact reconstruction
of a
function from its wavelet transform (for the Morlet wavelet it equals to
0.776) [17]. Once the average PS for each of the studied EEG bands is calculated
for each EEG channel and task, we have a high number feature vectors (bands x
channels) per task (class), representing each participant (subject), which is actu-
ally the time-scale-averaged PS (Global PS - Fig. 3.2 - Step 1) over the band of
interest.
δ ( · )
 
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