The properties of the DTFT are similar to those for the DFT and are important
in the analysis and interpretation of long signals. The main properties are
given here using the notation that the DTFT of a complex sequence
x
(
n
)
x
(
n
)
is
ℱ
{
x
(
n
)
}
=
X
(
ω
)
ℱ
{
x
(
n
)
}
=
X
(
ω
)
.
-
Linear Operator:
ℱ
{
x
+
y
}
=
ℱ
{
x
}
+
ℱ
{
y
}
ℱ
{
x
+
y
}
=
ℱ
{
x
}
+
ℱ
{
y
}
-
Periodic Spectrum:
X
(
ω
)
=
X
(
ω
+
2
π
)
X
(
ω
)
=
X
(
ω
+
2
π
)
-
Properties of Even and Odd Parts:
x
(
n
)
=
u
(
n
)
+
j
v
(
n
)
x
(
n
)
=
u
(
n
)
+
j
v
(
n
)
and
X
(
ω
)
=
A
(
ω
)
+
j
B
(
ω
)
X
(
ω
)
=
A
(
ω
)
+
j
B
(
ω
)
u
u
v
v
A
A
B
B
|
X
|
|
X
|
θ
θ
even
0
even
0
even
0
odd
0
0
odd
even
0
0
even
0
even
even
π
/
2
π
/
2
0
odd
odd
0
even
π
/
2
π
/
2
-
Convolution: If non-cyclic or linear convolution is defined
by:
y
(
n
)
=
h
(
n
)
*
x
(
n
)
=
∑
m
=
−
∞
∞
h
(
n
−
m
)
x
(
m
)
=
∑
k
=
−
∞
∞
h
(
k
)
x
(
n
−
k
)
y
(
n
)
=
h
(
n
)
*
x
(
n
)
=
∑
m
=
−
∞
∞
h
(
n
−
m
)
x
(
m
)
=
∑
k
=
−
∞
∞
h
(
k
)
x
(
n
−
k
)
then
ℱ
{
h
(
n
)
*
x
(
n
)
}
=
ℱ
{
h
(
n
)
}
ℱ
{
x
(
n
)
}
ℱ
{
h
(
n
)
*
x
(
n
)
}
=
ℱ
{
h
(
n
)
}
ℱ
{
x
(
n
)
}
-
Multiplication: If cyclic convolution is defined
by:
Y
(
ω
)
=
H
(
ω
)
∘
X
(
ω
)
=
∫
0
T
H
˜
(
ω
−
Ω
)
X
˜
(
Ω
)
ⅆ
Ω
Y
(
ω
)
=
H
(
ω
)
∘
X
(
ω
)
=
∫
0
T
H
˜
(
ω
−
Ω
)
X
˜
(
Ω
)
ⅆ
Ω
ℱ
{
h
(
n
)
x
(
n
)
}
=
1
2
π
ℱ
{
h
(
n
)
}
∘
ℱ
{
x
(
n
)
}
ℱ
{
h
(
n
)
x
(
n
)
}
=
1
2
π
ℱ
{
h
(
n
)
}
∘
ℱ
{
x
(
n
)
}
-
Parseval:
∑
n
=
−
∞
∞
|
x
(
n
)
|
2
=
1
2
π
∫
−
π
π
|
X
(
ω
)
|
2
ⅆ
ω
∑
n
=
−
∞
∞
|
x
(
n
)
|
2
=
1
2
π
∫
−
π
π
|
X
(
ω
)
|
2
ⅆ
ω
-
Shift:
ℱ
{
x
(
n
−
M
)
}
=
X
(
ω
)
e
−
j
ω
M
ℱ
{
x
(
n
−
M
)
}
=
X
(
ω
)
e
−
j
ω
M
-
Modulate:
ℱ
{
x
(
n
)
e
j
ω
0
n
}
=
X
(
ω
−
ω
0
)
ℱ
{
x
(
n
)
e
j
ω
0
n
}
=
X
(
ω
−
ω
0
)
-
Sample:
ℱ
{
x
(
K
n
)
}
=
1
K
∑
m
=
0
K
−
1
X
(
ω
+
L
m
)
ℱ
{
x
(
K
n
)
}
=
1
K
∑
m
=
0
K
−
1
X
(
ω
+
L
m
)
where
N
=
L
K
N
=
L
K
-
Stretch:
ℱ
{
x
s
(
n
)
}
=
X
(
ω
)
ℱ
{
x
s
(
n
)
}
=
X
(
ω
)
,
for
−
K
π
≤
ω
≤
K
π
−
K
π
≤
ω
≤
K
π
where
x
s
(
K
n
)
=
x
(
n
)
x
s
(
K
n
)
=
x
(
n
)
for integer
n
n
and zero otherwise.
-
Orthogonality:
∑
n
=
−
∞
∞
e
−
j
ω
1
n
e
−
j
ω
2
n
=
2
π
δ
(
ω
1
−
ω
2
)
∑
n
=
−
∞
∞
e
−
j
ω
1
n
e
−
j
ω
2
n
=
2
π
δ
(
ω
1
−
ω
2
)