booklet format - inaf iasf bologna
booklet format - inaf iasf bologna
booklet format - inaf iasf bologna
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Temporal Data Analysis A.A. 2011/2012<br />
Proof.<br />
3.3.3 Autocorrelation<br />
H j = 1 N<br />
= 1 N<br />
= 1 N<br />
Here we have {g k } = {f k }, which leads to<br />
N−1 ∑<br />
k=0<br />
N−1<br />
∑<br />
l=0<br />
N−1<br />
∑<br />
l=0<br />
1<br />
N<br />
N−1 ∑<br />
l=0<br />
1<br />
N−1 ∑<br />
f l<br />
N<br />
k=0<br />
f l G ∗ j W −j l<br />
N<br />
f l g ∗ l+k W −k j<br />
N<br />
g ∗ l+k W −k j<br />
N<br />
= F j G ∗ j<br />
and<br />
h k ≡ (f ⋆ f ) k = 1 N<br />
N−1 ∑<br />
l=0<br />
f l × f ∗<br />
l+k<br />
(3.24)<br />
{f k } ↔ {F j }<br />
{h k } = {(f ⋆ f ) k } ↔ {H j } = {F j × F ∗ j } = {|F j | 2 }<br />
(3.25)<br />
In other words: the Fourier transform of the autocorrelation of {f k } is the modulus squared of<br />
the Fourier series {F j } or its power representation.<br />
3.3.4 Parseval Theorem<br />
We use (3.24) for k = 0, that is h 0 , and get on the one side:<br />
h 0 = 1 N<br />
N−1 ∑<br />
l=0<br />
|f l | 2 (3.26)<br />
On the other hand, the inverse trans<strong>format</strong>ion of {H j }, especially for k = 0, results in (see (3.11b))<br />
Put together, this gives us the discrete version of Parseval theorem:<br />
1<br />
N<br />
N−1 ∑<br />
h 0 = |F j | 2 (3.27)<br />
N−1 ∑<br />
l=0<br />
j =0<br />
|f l | 2 N−1 ∑<br />
=<br />
j =0<br />
|F j | 2 (3.28)<br />
52 M.Orlandini