Digital Signal Processing Reference
In-Depth Information
Finally, if x
[
n
]
is real and symmetric, then the DTFT is real:
e j ω )
[
]
[
]=
[
] ⇐⇒
(
x
n
, x
n
x
n
X
(4.52)
l g r , y i d . , © , L s
while, for real antisymmetric signals we have that the DTFT is purely imagi-
nary:
Re X
e j ω ) =
x
[
n
]
, x
[
n
]=
x
[
n
] ⇐⇒
(
0
(4.53)
Linearity and Shifts. The DTFT is a linear operator:
DTFT
←→ α
e j ω )+ β
e j ω )
α
x
[
n
]+ β
y
[
n
]
X
(
Y
(
(4.54)
A shift in the discrete-time domain leads to multiplication by a phase term
in the frequency domain:
DTFT
←→ e −j ω n 0 X ( e j ω )
x [ n−n 0 ]
(4.55)
while multiplication of the signal by a complex exponential (i.e. signal mod-
ulation by a complex “carrier” at frequency ω 0 )leadsto
X e j ( ω ω 0 )
DTFT
←→
e j ω 0 n x
[
n
]
(4.56)
which means that the spectrum is shifted by
ω 0 .Thislastresultisknownas
the modulation theorem .
Energy Conservation. TheDTFT satisfies the Plancherel-Parseval equal-
ity:
x
] =
X
e j ω )
1
2
e j ω )
[
n
]
, y
[
n
(
, Y
(
(4.57)
π
and L 2 [ π
π ] :
or, using the respective definitions of inner product for
2 ( )
,
π
1
2
x [
X (
e j ω )
e j ω )
]
[
]=
(
ω
n
y
n
Y
d
(4.58)
π
n
= −∞
π
(note the explicit normalization factor 1
/
2
π
). The above equality specializes
into Parseval's theorem as
π
x
]
X
e j ω )
1
2
2
2
[
n
=
(
d
ω
(4.59)
π
n
= −∞
π
which establishes the conservation of energy property between the time and
the frequency domains.
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