yt=∫−∞∞
V
ω
t−τhτd
τ
=∫−∞∞hτeiω(t−τ)d
τ
=eiωt∫−∞∞hτe−(iωτ)d
τ
=Hωeiωt
y
t
τ
V
ω
t
τ
h
τ
τ
h
τ
ω
t
τ
ω
t
τ
h
τ
ω
τ
H
ω
ω
t
(1)
where
Hω
H
ω
is the
eigenvalue (scale factor) and
eiωt
ω
t
is
V
ω
t
V
ω
t
, which is the
eigenfunction.
Summary: Figure 2.
Hω=|Hω|ei∡Hω
H
ω
H
ω
∡
H
ω
(2)
where
|Hω|
H
ω
changes the amplitude of
eiωt
ω
t
and
ei∡Hω
∡
H
ω
changes the phase of
eiωt
ω
t
.
output=|Hω|ei(ωt+∡Hω)
output
H
ω
ω
t
∡
H
ω
(3)