Before we introduce truly non-Gaussian detection strategies, we
need to discuss the structure of the detector when the noise
amplitude distribution is known. From the results presented while
solving the general model evaluation problem, we find that the
likelihood ratio test for statistically independent noise values is
∑l=0L-1lnpnrl-
s
1
l-lnpnrl-
s
0
l
≷
ℳ
0
ℳ
1
γ
l
L
1
0
p
n
r
l
s
1
l
p
n
r
l
s
0
l
≷
ℳ
0
ℳ
1
γ
The term in braces is
ϒ
l
ϒ
l
, the sufficient statistic at the
l
th
l
th
sample. As LL is usually large and
each term in the summation is statistically independent of the
others, the threshold γγ is
found by approximating the distribution of the sufficient
statistic by a Gaussian (the Central
Limit Theorem again). Computing the mean and variance of
each term, the false-alarm probability is found to be
P
F
=Qlnη-∑E
ϒ
l
|
ℳ
0
∑σ
ϒ
l
|
ℳ
0
2
P
F
Q
η
ℳ
0
ϒ
l
ϒ
l
|
ℳ
0
This general result applies to any assumed noise density,
including the Gaussian. The matched filter answer derived
earlier is contained in the decision rule given above.
A matched-filter-like answer also results when small
signal-to-noise ratio problems are considered for
any amplitude distribution Kassam pp. 5-8, Spaulding, Spaulding and
Middleton). Assume that
lnpnrl-sl
p
n
r
l
s
l
, considered as a function of the signal value
sl
s
l
, can be expressed in a Taylor series centered at
rl
r
l
.
lnpnrl-sl=lnpnrl-ddnlnpnn|n=rlsl+12d2dn2lnpnn|n=rls2l+…
p
n
r
l
s
l
p
n
r
l
n
r
l
n
p
n
n
s
l
1
2
n
r
l
n
2
p
n
n
s
l
2
…
In the small signal-to-noise ratio case,
second and higher order terms are neglected, leaving the
decision rule
∑l=0L-1-ddnlnpnn|n=rl
s
1
l+ddnlnpnn|n=rl
s
0
l
≷
ℳ
0
ℳ
1
γ
l
L
1
0
n
r
l
n
p
n
n
s
1
l
n
r
l
n
p
n
n
s
0
l
≷
ℳ
0
ℳ
1
γ
This rule says that in the small signal case, the sufficient
statistic for each signal is the result of the match-filtering
the result of passing the observations through a front-end
memoryless non-linearity
-ddxlnpnx
x
p
n
x
, which depends only on noise
amplitude characteristics (see Figure 1).
Because of the presence of the matched filter and the
relationship of the matched filter to Gaussian noise problems,
one might presume that the nonlinearity serves to transform each
observation into a Gaussian random variable. In the case of the
zero-mean Gaussian noise,
-ddxlnpnx=xσ2
x
p
n
x
x
σ
2
. Interestingly, this Gaussian case is the
only instance where the "non-linearity" is
indeed linear and yields a Gaussian output. Now consider the
case where the noise is Laplacian (
pnn=12σ2ⅇ-|n|σ22
p
n
n
1
2
σ
2
n
σ
2
2
). The detector's front-end transformations is
-ddxlnpnx=signxσ22
x
p
n
x
sign
x
σ
2
2
. This non-linearity is known as an infinite
clipper and the output consists only
of the values
±1σ22
±
1
σ
2
2
, not a very Gaussian quantity.
-
S.A. Kassam. (1988). Signal Detection in Non-Gaussian Noise. New York: Springer-Verlag.
-
A.D. Spaulding. (1985). Locally optimum and suboptimum detector performance in a non-Gaussian interference environment. IEEE Trans. Comm., COM-33, 509-517.
-
A.D. Spaulding and D. Middleton. (1977). Optimum reception in an impulsive interference environment--Part I: Coherent detection. IEEE Trans. Comm., COM-25, 910-923.