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8.3 Wavelets
A wavelet ψ ( t ) is a function in the L 2 ( IR ) space over the real line IR that it
satisfies the following conditions.
The admissibility condition C ψ must remain finite, i.e.,
C ψ = +
−∞
| ψ ( ω )
2
|
dω <
,
(8.20)
|
ω
|
where ψ ( ω ) is the Fourier transform of ψ ( t ). ψ ( ω )= +
−∞
ψ ( t ) e −iωt
dt .
| ψ ( ω )
2 is the total power contained in ψ ( t )and C ψ is, therefore, the
total power per every frequency component present in ψ ( t ).
|
Its Fourier transform must be zero when the frequency is zero. This means
when ω =0,
ψ ( ω )= ψ (0) = 0 .
As a result, we obtain +
−∞
ψ ( t ) dt =0. ψ ( t ) dt is the area under the
curve ψ ( t ). Since it is zero, ψ ( t ) must change its sign, i.e., ψ ( t ) must be
oscillatory in nature or will have a wavelike behavior.
Since the sum of the power per every frequency component is finite, we
must have | ψ ( ω )
2
|
1
|
0 when ω
0. Now, ω
0 implies
| →∞
.
|
ω
|
ω
Therefore, to have
| ψ ( ω )
2
|
0 ,
|
ω
|
| ψ ( ω )
|
2
we must have
0 with a faster rate. Such a basic wavelet is
called a mother wavelet.
The mother wavelet represents a family of functions with two parameters: one
of them is for position and the other one is for frequency. In other words, the
family of functions is
1
|
ψ ( t
b
ψ a,b ( t )=
) ,
a
a
|
where a
=0and b
IR .
8.3.1 Continuous Wavelet Transform
Let us consider the family of functions
1
ψ ( t
b
ψ a,b ( t )=
) ,
(8.21)
a
|
a
|
 
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