X
c
s=∫-∞∞
x
c
tⅇ-ⅈωtdt
X
c
s
t
x
c
t
ω
t
(1)
s∈ℂ
s
X
c
ⅈΩ=∫-∞∞
x
c
tⅇ-ⅈΩtdt
X
c
Ω
t
x
c
t
Ω
t
(2)
t∈ℝ
t
Ω∈ℝ
Ω
X
c
t=12π∫-∞∞
x
c
Ωⅇ-ⅈΩtdΩ
X
c
t
1
2
Ω
x
c
Ω
Ω
t
(3)
Notes:
-
X
c
Ω
X
c
Ω
is the Laplace Transform evaluated at
s=ⅈΩ
s
Ω
.
-
When the
X
c
t
X
c
t
is "smooth",
X
c
Ω
X
c
Ω
is concentrated around
Ω=0
Ω
0
and dies off as
|Ω|→∞
Ω
.
-
When
X
c
t
X
c
t
is real valued,
X
c
Ω
X
c
Ω
is conjugate symmetric.
-
When
X
c
t
X
c
t
is "bandlimited",
X
c
Ω=0
X
c
Ω
0
for all
|Ω|>
Ω
0
Ω
Ω
0
,
where
Ω
0
Ω
0
is the cutoff frequency.