A COMPARATIVE STUDY OF SOME TIME-FREQUENCY DISTRIBUTIONS USING
RENYI CRITERION
D. Boutana*, M. Benidir **, F. Marir *** and B. Barkat****
* Department of Electronic, Faculty of Science, University of Jijel PO. Box 98, JIJEL, ALGERIA
e–mail: daoud.boutana@mail.com
** Université Paris-Sud, Laboratoire des Signaux et Systèmes, Supelec, Plateau de Moulon 91192 Gif-sur-Yvette, FRANCE,
e–mail : messaoud.benidir@lss.supelec.fr
***Department of Electronic, Faculty of Science, University of Constantine, Constantine, ALGERIA
e-mail: F.Marir@yahoo.fr
**** Nanyang Technological University, School of Electrical and Electronic Engineering, SINGAPORE
e–mail : ebarkat@ntu.edu.sg
ABSTRACT
The paper presents a quantitative comparison study of some
time-frequency distributions i.e. (TFDs). The comparison
is in terms of a criterion known as the Renyi measure. The
assessment of the TFDs is accomplished by evaluating the
Rényi measure which yields the best time-frequency resolution. We show, using synthetic as well as real-life data, that
a recently proposed TFD outperforms existing TFDs. In
particular, we show that this proposed TFD presents a high
time-frequency resolution while suppressing the undesirable cross-terms.
1. INTRODUCTION
In this paper, we present a quantitative comparative study
between some existing time-frequency distributions (TFDs)
and a recently proposed one [1] in the analysis of multicomponent signals. In the comparison, we consider the crossterms suppression and the high energy concentration of the
signal around its instantaneous frequency (IF).The widely
used spectrogram (SP), which is in general a cross-terms free
TFD, suffers from the undesirable trade-off between time
resolution and frequency resolution [2], [3], [4], and [5]. On
the other hand, the Wigner-Ville distribution (WVD) has a
high time-frequency resolution but is known to suffer from
the presence of cross-terms [2]. To address the problem of
cross-terms suppression, while keeping a high timefrequency resolution, other TFDs have been proposed.
Among these, one can cite the Zhao-Atlas-Marks distribution (ZAMD) [6], the B-distribution (BD) [7] and the Modified B-distribution (MBD) [8], just to name a few. In the sequel, we will compare these reduced cross-terms TFDs to a
newly proposed TFD, inspired from the Butterworth kernel
quadratic TFD [9]. The comparison is performed by evaluating the Rényi criterion for each of the considered TFDs.
Since these TFDs are function of some parameters, we first
obtain the optimal parameters in terms of the minimal values
of the Rényi information for each individual one. Then, we
compare them to each other. Synthetic as well as real-life
data are used in this comparative study. The paper is organized as follows: In Section 2, we give a brief theoretical
background of the various TFDs used in the comparison and
present some properties of the comparison tool (i.e., the Rényi information criterion). In Section 3, we present some
simulations results as well as a discussion. Section 4 concludes the paper.
2. QUADRATIC TIME-FREQUENCY
DISTRIBUTION
Quadratic, a.k.a. bilinear or Cohen’s, TFDs constitute a powerful tool in the analysis of non-stationary signals, i.e., signals whose frequency contents vary with time. Many of
these representations are invariant to time and frequency
translations and can be considered as energy distribution in
the time-frequency plane. The quadratic class can be expressed as [2, 4].
C x (t,f )= ∫∫∫e
Φ x (ξ,τ )x(u + 2τ )x* (u − 2τ )dud τdξ
j2π(ξt − ξf − fτ )
(1)
where x (t) represents the analytical form of signal under
consideration and Φx(ξ,τ) is called the kernel of the distribution. All the integrals are from - ∞ to + ∞ , unless otherwise
stated. A choice of a particular kernel function yields a particular quadratic TFD with its own specificities [2], [3]. All
the reduced cross-terms TFDs mentioned earlier are members of the quadratic class. In particular, the kernel of the
Butterworth kernel is given by [9]
Φ x (ξ , τ )=
ξ
1+
σξ
1
2N
τ
στ
2M
(2)
This kernel, which is a general form of the exponential
kernel, is considered as a low-pass filter in the ambiguity
domain. A suitable choice of the parameters N, M, σ ξ and
σ τ helps remove the cross-terms from the TFD, in the
analysis of a multicomponent signal.
A recently proposed TFD, inspired from the Butterworth
kernel, was shown to possess a good trade-off between crossterms suppression and high time-frequency resolution [1].
This TFD kernel is expressed as
πσξ
Φ x (ξ , τ )=
ξ
1+
σ
ξ
2N
.
1
2M
τ
1+
στ
(3)
Using the inverse Fourier Transform and fixing N equal to
unity, we obtain the time-lag kernel expression given by
Φ x (t , τ )=
1
τ
1 +
στ
2M
exp ( − πσ ξ t )
(4)
( ) ( )e
Now, by substituting expression (3) in Equation (1), we obtain the proposed TFD expression as
Cx (t,f) = ∫∫
1
*
−πσξ s−t
x s+ τ x s−τ
2M e
2
2
1+ τ2
στ
− j2 π f τ
dsd τ
(5)
In this comparison study, we have used the Rényi information of order α defined as:
α
R α = 1 −1α log2 ∫∫C x (t,f )dt df
(6)
α: Rank of the Rényi measure, α ≥ 2 .
This criterion was used in [10], [11], and [12] to evaluate the
complexity of a signal in the time frequency plane. Four
schemes have been studied in [12] but both of them using the
normalized form versus volume have been proved to have
useful properties. The normalization operation assures that
the TFD behave like a probability density function (pdf). So
minimising the Rényi entropy for a given TFD is equivalent
to maximizing its concentration, peakiness and resolution
[13]. Then the best parameters of kernel for TFD with respect to the minimal value of the Rényi will give a good
localization of the energy. Recently in [14] the performance
of minimum entropy kernels for best TFDs and component
counting is also demonstrated. In our study we have used the
second and the third order of Rényi entropy with volume
normalized. Moreover the discrete-time formulation of the
Rényi entropy for TFD [12] with normalization volume is
given by:
C(n,k )
(7)
∑ K
N
n = −N ∑ k = −K ∑ n = −N C(n,k )
where n and k are variables for discrete-time and discrete
frequency respectively , N and K are number of samples in
time and frequency respectively.
K
RVα = 1 log 2 ∑
1−α
k = −K
N
α
3. EXAMPLES AND DISCUSSIONS
All analysis is done using third order Rényi entropy RV3
since it has been proved [10-11] that is the well choice for
measuring time-frequency uncertainty. We have particularly
used the normalized scheme versus the volume which has
been used for adaptive kernel design [11, 12]. The goal is to
Fig. 1. TFDs results of signal given in example 1.
TABLE I
OPTIMAL VALUES OF THE KERNEL PARAMETER
TFD
nh
RV2
RV3
WVD
SP
ZAMD a=2
Proposed TFD σξ=0.05
MBD β=0.05
89
111
111
85
5.8912
5.0359
5.4923
4.2892
4.5840
5.9936
4.8583
5.2780
4.0895
4.2538
TABLE II
OPTIMAL VALUES OF THE KERNEL PARAMETER FOR BAT
SIGNAL ANALYSIS
ZAMD MBD
TFD WVD SP
Proposed TFD
nh=65 nh=85 nh=65
nh=45 σξ=0.05
a=2
β=0.05
2.9961
RV3 4.6253 2.1148 4.1835 3.3090
(a)
(b)
Fig. 2. Left: Slices taken at time instant n=256 for (a) WVD, (b) SP
(c) ZAMD (d) Proposed TFD (e) MBD. Right: Performance comparison
between SP (dashed line) and the proposed TFD (solid line). Horizontal
axis shows frequency in Hz.
find based on Rényi measure the best parameters that can
give better TFDs results. Then achieved comparison and
interpretation between each TFDs. The data window length
which controls the size of the kernel used for analysis is
noted nh. Some results of TFDs have been realized by TFSA
[15] except for the proposed TFD.
3.1. Example 1: Sinusoidal and linear FM components
In this example, the synthetic signals consist of two components the first is sinusoidal FM component and the second
is linear FM given by:
x(t ) = cos (−50 cos (πt) +10πt 2 + 70πt) +cos (25πt 2 +180πt)
A sampling frequency is equal to fs=256 Hz with a signal
length equal to 512. Table I shows the optimal parameters
corresponding to the minimal values of the Rényi measure
for all TFDs. Each result of TFDs has been obtained after
several variations of optional parameters. All optimized
TFDs are represented in figure 1, where horizontal axis
shows the frequency and vertical axis is the time. The Left
part of figure 2 shows slices taken at the same time instant
n=256 for different TFDs with optimal parameters when the
right part shows slices taken at the same time instant n=256
for the SP and the proposed TFD.
3.2. Example 2: Bat signal.
In this example, the real-life signal consisting of Bat chirp
signal1 digitized at 2.5 microsecond echolocation pulse
emitted by the Large Brown Bat, Eptesicus Fuscus. There
are approximate 400 samples; the sampling period was 7
microseconds, the signal length used is equal to 512 and
the sampling frequency is fixed equal to fs =143.72 KHz.
Also, the same TFDs used in the first example are considered here. To find the optimal TFD for resolving the components of the signal we first find the optimal values of the
1
The authors wish to thank Curtis Condon, Ken White, and Al Feng of the
Beckman Institute of the University of Illinois for the bat data and for permission to use it in this paper.
(d)
(c)
Fig. 3. Evolution of RV3 versus nh for (a) ZAMD (b) MBD (c) Proposed TFD and (d) Optimal values of RV3 for all TFDs.
Fig. 5. Slices taken at the same time n=150 (left) and n=250 (right) for
(a) WVD, (b) SP, (c) ZAMD, (d) BD, (e) MBD, (f) Proposed TFD.
Horizontal axis shows frequency in KHz.
TFDs kernel parameters using Rényi criterion. The values of
RV3 have been measured for all TFDs versus each proper
parameter. Different values of window lengths and optional
parameters have been used in the evaluation of the Rényi
measure. All the minimal values of Rényi that represent the
best time-frequency concentration and elimination crossterms have been summarized on table II. We can see also the
optimal value of the kernel parameter for each TFDs. The
variations of RV3 versus the window length for each TFDs
can be seen in figure 3. The results of TFDs using the optimal parameters are represented in Figure 4. We take slices of
the TFDs at the time instants n= 150 and n=250 (recall that
n= 1, 2…512) and we plot the normalized amplitudes of
these slices in figure 5. We can see in left part of this figure
that the first and the second components have appeared without cross-terms. In the right part we can see the second component and the third component without cross-terms. Also we
can remark that the results of the proposed TFD show a better performance, in terms of frequency resolution. However
the highest performance is achieved by the MBD and the
proposed TFD for signal in consideration. Also we can remark that the proposed TFD not only can successfully appear
the third components (the weakest) but it has the best resolution i.e (narrower main-lobe and smaller side-lobes) compared to all the other considered distributions.
Fig. 4. Bat signal analysis by (a) WVD,(b) SP, (c) ZAMD , (d) BD σ=0.05 nh =45, (e) MBD β=0.05 nh =65 and (f) Proposed TFD σξ=0.05 nh =45.
Horizontal axis show frequency in KHz, vertical axis show time versus number of samples.
4. CONCLUSION
In this paper, we presented a quantitative comparative study
of some quadratic TFDs using synthetic and real-life bat
signal. We have used some distributions known for their
high cross-terms suppression property in terms of trade-off
between cross-terms suppression and high energy concentration in the time-frequency domain. The optimal parameters
of all TFDs have been selected based on the Rényi criterion.
Our study have show that the proposed TFD exhibits high
resolution and very little interference terms between the
signal components both on simulated or real signal.
[7]
[8]
[9]
[10]
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Developed by Professor Boualem Boashash, Signal
Processing Research Laboratory Queensland University of Technology GPO Box 2434, Brisbane 4001
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