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Signal Processing
Volume 76, Issue 3, August 1999, Pages 323-326
 
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doi:10.1016/S0165-1684(99)00053-5    How to Cite or Link Using DOI (Opens New Window)
Copyright © 1999 Published by Elsevier Science B.V. All rights reserved.

Fast communication

On LLRT detection of deterministic signals in multiplicative noise

Denis A. Orlova, Victor I. Turchina and Alex B. GershmanCorresponding Author Contact Information, E-mail The Corresponding Author, b

a Institute of Applied Physics RAS, Nizhny Novgorod, Russia b Department of Electrical and Computer Engineering, McMaster University, Ontario, Canada

Received 11 May 1998.
Available online 29 July 1999.

Abstract

The LLRT detector for a known deterministic signal in the presence of multiplicative noise is studied. An interesting property of this “multiplicative” detector is discovered. For the exponential class of noise covariances, it is shown that an unrestricted increase of output SNR (detection index) can be achieved when increasing the sampling rate. Such effect does not occur in the case of LLRT detector in the presence of additive noise, where the detection index is limited by the noise correlation time.

Author Keywords: LLRT detector; Multiplicative noise; Sampling rate

Article Outline

1. Introduction
2. Problem formulation and LLRT detector
3. Performance analysis
4. Sampling rate and performance
References

1. Introduction

Signal detection/estimation in multiplicative noise is an important problem in radar, sonar and image processing [1, 2, 5, 6 and 7]. Below, we consider the log-likelihood ratio test (LLRT) detector for a known deterministic signal observed in multiplicative noise. An interesting property of this detector is discovered: for the exponential class of noise covariances, an unrestricted increase of output SNR can be achieved when increasing the sampling rate. In the case of additive noise, the LLRT detector is known to have quite different behavior, i.e., when increasing the sampling rate, the detection index is known to be severely restricted by the noise correlation time.

2. Problem formulation and LLRT detector

Let the samples of the known deterministic complex signal yi be observed in the presence of multiplicative noise, i.e.,

(1)
xiiyi, i=1,2,…,N ,
where ξi is assumed to be a complex zero-mean Gaussian random process. Eq. (1) in vector notation is expressed as

(2)
x= ,
where x=(x1, x2, …, xN)T, ξ=(ξ1, ξ2, …, ξN)T, Y=diag{y1, y2, …, yN}, and (·)T stands for transpose. In the most general statement, the detection problem can be formulated as deciding between two hypotheses

(3)
Image
where the signal matrices Y0 and Y1 are known a priori. Let the covariance matrix of multiplicative noise

(4)
Q=E{ξξH}
be of arbitrary structure but be known a priori (for example, measured prior to processing [5]). Here, (·)H stands for Hermitian transpose.

The LLRT is given by

(5)
Λ(x)=log p(x|H1)−log p(x|H0)>ν ,
where p(x|Hi), i=0,1, is the probability density function of the received data under the hypothesis Hi, and ν is a threshold. The covariance matrix of the observed signal (2) is given by

(6)
Image
From (5) and (6), we obtain

(7)
Image
where the constant terms (not depending on x) are omitted. In what follows, let us assume that

(8)
Y0=I, Y1=I+S ,
where I is the identity matrix, and S=diag{s1, s2, …, sN} is a discrete-time version of known deterministic signal s(t) satisfying the weakness assumption |s(t)|much less-than1. This model is quite typical for the long-path underwater transmission [3]. The weak (known) perturbations si occur when an inhomogeneity crosses the transmission path.

Let us use the following matrix expansion:

(9)
(I+S)−1=IS+S2S3+cdots, three dots, centered .
Neglecting the second- and higher-order terms, we obtain from (7), (8) and (9) the approximate LLRT

(10)
Λ(x)similar, equalsxH(SHQ−1+Q−1S)x .

3. Performance analysis

The detection performance is measured in terms of the receiver operating characteristic (ROC), or, alternatively, in terms of the detection index [4]

(11)
Image
where

(12)
Si=E{Λ(x)}|Hi, Di=var{Λ(x)}|Hi, i=0, 1 .
In fact, Eq. (11) represents the output SNR of the detector. From (6) and (7), it follows that

(13)
E{Λ(x)}=tr{R(R0−1R1−1)} .

Noting that for a zero-mean Gaussian process

(14)
E{xixk*xlxm*}=[R]ik[R]lm+[R]im[R]lk ,
we obtain that

(15)
Image
From (12), (13) and (15), we have

(16)
S0S1=2N−tr{R0R1−1+R1R0−1} ,


(17)
D0=N−2 tr{R0R1−1}+tr{(R0R1−1)2} .
Finally, the detection performance is given by (11), (16) and (17). For the approximate log-likelihood ratio (10), the detection index can be simplified to

(18)
Image

4. Sampling rate and performance

Let us study how the detection index (18) depends on the sampling rate. Assume that the input signal x is observed within the fixed interval [ta, tb] with the uniform sampling

(19)
Image
Assume also that the noise covariance matrix (4) belongs to the exponential class, i.e., let

(20)
[Q]nmξ2r|nm|, r=exp(−Δ/τc) ,
where σξ2 and τc are the noise variance and its correlation time, respectively. Exponential covariances are widely used for the modeling of multiplicative noise in sonar applications [5].

Let us find the limit of η (18) for N→∞ (or, equivalently, Δ→0). From Eq. (18) it follows that, first of all, we should evaluate the term

(21)
FUV=tr{UQVQ−1} ,
with arbitrary diagonal matrices

(22)
U=diag {u1, u2, …, uN}, V=diag {v1, v2, …, vN} .

Exploiting a 3-diagonal representation for the inverse of Eq. (20) [2]

(23)
Image
Eq. (21) becomes

(24)
Image
Using a Taylor series expansion,

(25)
Image
and the following representation of the Riemann sum,

(26)
Image
we find that

(27)
Image
Hence, we obtain from (18) and (27) that

(28)
Image
Therefore, the detection performance can increase unlimitedly (proportionally to Image ) if the sampling rate increases (i.e., Δ→0), provided the observing interval is fixed. Obviously, this property does not hold in the presence of additive noise. To demonstrate this fact, consider the following signal model with additive zero-mean Gaussian noise:

(29)
xi=sii, i=1, 2, …, N .
The detection index after the LLRT detector for additive noise is given by [4] Image , where s=(s1, s2, …, sN)T. Proceeding in the same manner as for the multiplicative noise case, we obtain that in the additive noise case

(30)
Image
Hence, unlike the multiplicative noise case, the detection index in the additive noise case is limited by the constant terms in Eq. (30). In particular, if Δ<τc, then the further increase of the sampling rate cannot improve the performance more.

References

1. O. Besson and F. Castanié. On estimating the frequency of a sinusoid in autoregressive multiplicative noise, Signal Processing 30 (January 1993), pp. 65–83. Article | PDF (1077 K) | View Record in Scopus | Cited By in Scopus (22)

2. A.B. Gershman, D.A. Orlov, V.I. Turchin, Detection of regular signals in the presence of multiplicative noise, in: Proc. 1st European Conf. on Signal Analysis and Prediction, Prague, June 1997..

3. J.A. Mercer, J.R. Booker, Long-range propagation of sound through oceanic mesoscale structures, Journal Geophys. Research 88 (C1) (1983) 689–699..

4. R.A. Monzingo, T.W. Miller, Introduction to Adaptive Arrays, Wiley, New York, 1980..

5. A. Paulraj and T. Kailath. Direction of arrival estimation by eigenstructure methods with imperfect spatial coherence of wave fronts, J. Acoust. Soc. Amer. 83 (March 1988), pp. 1034–1040.

6. A. Swami. Multiplicative noise models: Parameter estimation using cumulants, Signal Processing 36 (April 1994), pp. 355–373. Article | PDF (1274 K) | View Record in Scopus | Cited By in Scopus (23)

7. G. Zhou and G.B. Giannakis. Harmonics in multiplicative and additive noise: Cramer–Rao bounds, IEEE Trans. Signal Process. SP-43 (May 1995), pp. 1217–1231. View Record in Scopus | Cited By in Scopus (12)

Corresponding Author Contact Information Corresponding author; email: gershman@ieee.org


Signal Processing
Volume 76, Issue 3, August 1999, Pages 323-326
 
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