The forward and inverse Laplace transforms are defined as:
Fs=∫−∞∞fte−(st)d
t
F
s
t
f
t
s
t
(1)
ft=12πi∫a−i∞a+i∞Fsestd
s
f
t
1
2
s
a
a
F
s
s
t
(2)
substitute in
s=iω
s
ω
and let
a=0
a
0
(integrate along
iω
ω
axis in complex plane)
and we have:
Fiω=∫−∞∞fte−(iωt)d
t
F
ω
t
f
t
ω
t
(3)
ft=12π∫−∞∞Fiωeiωtd
ω
f
t
1
2
ω
F
ω
ω
t
(4)
In other words
Fiω=Fs|
s=iω
F
ω
s
ω
F
s
(5)
which explains the "
iω
ω
"
notation.
f∈L2R
f
L
2
but not
L′R
L
.
∫|ft|d
t
=∞
t
f
t
and
∫|ft|2d
t
<∞
t
f
t
2
.
f∈L′R
f
L
but not
L2R
L
2
.
∫|δt|d
t
=1
t
δ
t
1
and
∫|δt|2d
t
=∞
t
δ
t
2
.