Detection theory applies optimal model evaluation to signals
(Helstrom, Poor, van Trees).
Usually, we measure a signal in the presence of additive noise
over some finite number of samples. Each observed datum is of
the form
sl+nl
s
l
n
l
, where
sl
s
l
denotes the
l
th
l
th
signal value and
nl
n
l
the
l
th
l
th
noise value. In this and in succeeding sections of this
chapter, we focus the general methods of evaluating models.
For the moment, we assume we know the joint distribution of
the noise values. In most cases, the various models for the
form of the observations - the hypothesis - do not differ
because of noise characteristics. Rather, the signal component
determines model variations and the noise is statistically
independent of the signal; such is the specificity of
detection problems in contrast to the generality of model
evaluation. For example, we may want to determine whether a
signal characteristic of a particular ship is present in a
sonar array's output (the signal is known) or whether no ship
is present (zero-valued signal).
To apply optimal hypothesis testing procedures previously
derived, we first obtain a finite number
LL of observations
rl
r
l
,
l∈0…L-1
l
0
…
L
1
. These observations are usually obtained from continuous-time
observations in one of two ways. Two commonly used methods for
passing from continuous-time to discrete-time are known:
integrate-and-dump and
sampling. These techniques are illustrated in
Figure 1.
In this procedure, no attention is paid to the bandwidth of
the noise in selecting the sampling rate. Instead, the
sampling interval ΔΔ is
selected according to the characteristics of the signal
set. Because of the finite duration of the integrator,
successive samples are statistically independent when the
noise bandwidth exceeds
1Δ
1
Δ
Consequently, the sampling rate can be varied to some extent
while retaining this desirable analytic property.
Traditional engineering considerations governed the
selection of the sampling filter and the sampling rate. As
in the integrate-and-dump procedure, the sampling rate is
chosen according to signal properties. Presumably, changes
in sampling rate would force changes in the filter. As we
shall see, this linkage has dramatic implications on
performance.
With either method, the continuous-time detection problem of
selecting between models (a binary selection is used here for
simplicity)
ℳ
0
:
rt=
s0
t+nt
0≤t<T
ℳ
0
:
r
t
s0
t
n
t
0
t
T
ℳ
1
:
rt=
s1
t+nt
0≤t<T
ℳ
1
:
r
t
s1
t
n
t
0
t
T
where
sit
si
t
denotes the known signal set and
nt
n
t
denotes additive noise modeled as a stationary stochastic
process is converted into the discrete-time detection
problem
ℳ
0
:
r
l
=
s
l
0
+
n
l
0≤l<L
ℳ
0
:
r
l
s
l
0
n
l
0
l
L
ℳ
1
:
r
l
=
s
l
1
+
n
l
0≤l<L
ℳ
1
:
r
l
s
l
1
n
l
0
l
L
where the sampling interval is always
taken to divide the observation interval
T
:
L=TΔ
T
:
L
T
Δ
. We form the discrete-time observations into a
vector:
r=r0…rL-1T
r
r
0
…
r
L
1
. The binary detection problem is to distinguish
between two possible signals present in the noisy output
waveform.
ℳ
0
:
r=s0+n
ℳ
0
:
r
s
0
n
ℳ
0
:
r=s1+n
ℳ
0
:
r
s
1
n
To apply our model evaluation results, we need the probability
density of rr under
each model. As the only probabilistic component of the
observations is the noise, the required density for the
detection problem is given by
pr|
ℳ
i
r=pnr-si
p
r
ℳ
i
r
p
n
r
s
i
and the corresponding likelihood ratio by
Λr=pnr-s1pnr-s0
Λ
r
p
n
r
s
1
p
n
r
s
0
Much of detection theory revolves about interpreting this
likelihood ratio and deriving the detection threshold (either
thresholdthreshold or
γγ).
-
C. W. Helstrom. (1968). Statistical Theory of Signal Detection. (Second Edition). Oxford: Pergamon Press.
-
H. V. Poor. (1988). An Introduction to Signal Detection and Estimation. New York: Springer-Verlag.
-
H. L. van Trees. (1968). Detection, Estimation, and Modulation Theory, Part I. New York: John Wiley & Sons.