3.3 The One-Sided Laplace Transform 183
FIGURE 3.8
Poles (top right) of the Laplace
transform of the autocorrelation
c(t)=e−^2 |t|(top left), which is
noncausal. The ROC ofC(s)is the
region in between the poles, which
includes thejaxis. The spectrum
|C()|^2 corresponding toc(t)is
shown in the bottom plot—this is the
magnitude square of the Fourier
transform ofc(t).
− 20 − 10 0 10 20
0
0.2
0.4
0.6
0.8
1
Ω(rad/sec)
|C(
Ω
(^2) )|
− 5 0 5
0
0.2
0.4
0.6
0.8
1
t
c(
t)
− 2 0 2
− 1
−0.5
0
0.5
1
σ
jΩ
Thus, the system function is
H(s)=
1
s+ 1
+
1
−s+ 2
=
− 3
(s+ 1 )(s− 2 )
with a region of convergence the intersection of the regions of convergence of its components, or
the intersection of{(σ,):σ >−1,−∞< <∞}and{(σ,):σ <2,−∞< <∞}, or
{(σ,):− 1 < σ <2,−∞< <∞}
which is a sector of thes-plane that includes thejaxis. Thus,H(j)can be computed from its
Laplace transform. n