Proof
We
form
Then the condition (
Multiresolution
analysis
)-4 and
are evident. The orthogonality part of
(
Multiresolution analysis
)-5 follows
from the QMF conditions, see the proof of the proposition
(
Scaling equation 3
).
We now prove the condition
(
Multiresolution analysis
)-1.
By condition 1 and according to the section
(
Fourier transform of
delta function
),
For a general function
,
thus
From the formula
we
conclude
We take inverse Fourier transform of the above. The product becomes
convolution:
Thus we have the condition
(
Multiresolution
analysis
)-1:
We now verify the condition
(
Multiresolution analysis
)-3. It
suffices to show that
we
have
We start with the case of function
with compact
support:
We
estimate
for some
.
Note that
when
.
Then
and
converges because
.
Thus
The set of functions
with compact support constitutes a dense set in
and for each function on such dense set we
have
Hence, the above convergence result extends to all
by the following standard argument. Let
and
have compact support and
,
as
.
If
does not converge to zero then there is a subsequence
such that
is separated from zero. But then we arrive to contradiction because everything
on the RHS of
can be arbitrarily small.
The final task is to verify the condition
(
Multiresolution analysis
)-2. We need
to
show
Note
that
thus
or
According to the proposition
(
Fourier
transform of projection on span of
translates
),
We use the formula (
Property of
scale and transport
5
).
We assume that the function
has compact support and prove the statement. Then the general case follows by
density argument, similarly to the
above.
Note that if
is large enough and
has compact support then the only non-zero terms are those with
.
We make the change
.
Note that the sum has structure of integral as
.
The term
becomes zero,
becomes the variable of
integration:
where the last equality follows from the condition 2 and the propositions
(
QMF property 1
)-b and
(
Basic properties of Fourier
transform
)-3. We
continue
We make a change
.
Since
is finite,
has compact support and, thus,
is infinitely smooth. Hence,
where
and thus
.
Then, by
,
condition 2 and the proposition (
QMF property
2
)-a, we have
.
We make the reverse change of
variables.
We
obtained