In signal processing, a quadrature filter
q(t)
f(t)
q(t)=fa(t)=\left(\delta(t)+j\delta(jt)\right)*f(t)
If the quadrature filter
q(t)
s(t)
h(t)=(q*s)(t)=\left(\delta(t)+j\delta(jt)\right)*f(t)*s(t)
which implies that
h(t)
(f*s)(t)
Since
q
q
An ideal quadrature filter cannot have a finite support. It has single sided support, but by choosing the (analog) function
f(t)
This construction will simply assemble an analytic signal with a starting point to finally create a causal signal with finite energy. The two Delta Distributions will perform this operation. This will impose an additional constraint on the filter.
For single frequency signals (in practice narrow bandwidth signals) with frequency
\omega
\omega
h(t)=(s*q)(t)=
1 | |
\pi |
infty | |
\int | |
0 |
S(u)Q(u)eidu=
1 | |
\pi |
infty | |
\int | |
0 |
A\pi\delta(u-\omega) Q(u)eidu=
=A
infty | |
\int | |
0 |
\delta(u-\omega)Q(u)eidu= AQ(\omega)ei
|h(t)|=A|Q(\omega)|
This property can be useful when the signal s is a narrow-bandwidth signal of unknown frequency. By choosing a suitable frequency function Q of the filter, we may generate known functions of the unknown frequency
\omega