 Research
 Open Access
 Published:
On a new WignerVille distribution associated with linear canonical transform
EURASIP Journal on Advances in Signal Processing volume 2021, Article number: 56 (2021)
Abstract
Linear canonical transform as a general integration transform has been considered into WignerVille distribution (WVD) to show more powerful ability for nonstationary signal processing. In this paper, a new WVD associated with linear canonical transform (WVDL) and integration form of WVDL (IWVDL) are presented. First, the definition of WVDL is derived based on new autocorrelation function and some properties are investigated in details. It removes the coupling between time and time delay and lays the foundation for signal analysis and processing. Then, based on the characteristics of WVDL over timefrequency plane, a new parameter estimation method, IWVDL, is proposed for linear modulation frequency (LFM) signal. Two phase parameters of LFM signal are estimated simultaneously and the cross term can be suppressed well by integration operator. Finally, compared with classical WVD, the simulation experiments are carried out to verify its better estimation and suppression of cross term ability. Error analysis and computational cost are discussed to show superior performance compared with other WVD in linear canonical transform domain. The further application in radar imaging field will be studied in the future work.
Introduction
The classical WignerVille distribution (WVD), as an important and fundamental tool of timefrequency analysis, has been developed over the years in many engineering systems [1–6]. It can be also viewed as traditional Fourier transform (FT) kernel on autocorrelation function. Linear canonical transform (LCT) is a generalized integral transform of FT and fractional FT (FRFT) and defined as [7–9]
where
and parameter matrix \(A=[a\ \ b;\ c\ \ d], a, b, c, d \in \mathbb {R}\) and A=1. From (1) and (2), LCT can be reduced to be FT, FRFT, or other affine transform when A is chosen specially. LCT plays a major role in nonstationary signal processing, especially for detection and estimation of LFM signals, which has been developed into diverse application areas [10–13]. However, although LCT and WVD are important and effective tools in LFM signal processing, LCT cannot gather signal energy strongly like WVD and only classical WVD does not exploit phase feature of LFM signal fully. As a result, they display the poor performance under low signaltonoise ratio (SNR) for detection and estimation. In order to improve the performance of LFM signal detection and estimation, therefore, a series of WVD associated with LCT have been proposed by researchers, which are effective way and validated by some works [14–22].
The WVD associated with the LCT (LCWD) was first investigated from generalized transform domain perspective in [14] and the relations among some timefrequency distributions and linear canonical operators have been discussed. Along with this idea, the WVD associated with LCT has been studied in depth and widely [15–20, 22]. The WVD based on LCT (WDL) was first defined in time domain by replacing the kernel of classical FT with kernel of LCT [15]. Based on this notion, some basic properties were also derived. This WDL raised more analysis views of LFM signal in timelinear canonical frequency (LCF) plane and then was applied to estimating parameter of LFM signals. In [16], a new version of LCWD and its moment were investigated, which was applied to firstorder optical system. In the same year, a crossWVD for timefrequency analysis and generalized WVD for the estimation of quadratic frequency modulation signal were presented in LCT domain [17]. Afterwards, unified WVD in the LCT domain (UWDL) was proposed by substituting the classical autocorrelation function with a generalized autocorrelation function in [18], which unifies LCWD and WDL by nine free parameters. In order reduce parameter complexity of UWDL, two special cases of this UWDL were presented by less parameters [19, 20]. These unified WDL have more robust detection performance of LFM signal in noise environment than those in [14, 15] as well as the classical WVD [1]. However, autocorrelation function of LFM signal contains coupling between time and time delay, which is the essential phase characteristics and is not considered in above methods. For this, the author proposed a novel WVD associated with LCT in [21] and some basic properties were derived. This method can remove coupling and make energy distribution a straight line parallel to time axis, which was used to detect LFM signal theoretically. Nevertheless, there are other useful properties and better performance for parameter estimation of LFM signal based on this method that have not been developed.
For this purpose, the definition of WVD associated with LCT (WVDL) is derived by new autocorrelation function in LCT domain. The WVDL is able to represent and acquire characteristics of LFM signal using affine transform advantage of LCT to timefrequency plane. Then, other useful properties [23, 24] are investigated and proved in details including nonlinearity, linear canonical time shift, linear canonical modulation, dilation, reconstruction formula, and convolution. Based on above characteristics of energy distribution, a novel parameter estimation method, integration form of WVDL (IWVDL), is proposed, which estimate two phase coefficients of LFM simultaneously and suppress cross terms effectively for multicomponent LFM signal. Finally, to demonstrate superior estimation performance of LFM signal, the simulation experiments are carried out and the estimation error, computation cost and application are discussed.
The remainder of this paper is organized as follows: Preliminaries summarizes common notations and basic operators and then reviews existing WVD definitions in the Section 2. Section 3 presents a WVDL from a new point of view and derive some properties. Based on this definition, a new parameter estimation method IWVDL is proposed. Section 4 is the results and discussion about estimation performance and application of proposed method. Section 5 concludes this paper.
Preliminaries
Notations and operators
We will summarize some notations and review some basic operators in this subsection (Table 1).
Time Shift: For a complex signal \(x(t) \in L^{2}(\mathbb {R})\), a time shift operator T_{s} is given as
Modulation: For a complex signal \(x(t) \in L^{2}(\mathbb {R})\), a modulation operator \(\mathbf {M}_{u_{0}}\) is given as
Dilation: For a complex signal \(x(t) \in L^{2}(\mathbb {R})\), a dilation operator \(\mathbf {D}_{t_{0}}\) is given as
Linear canonical time shift: For a complex signal \(x(t) \in L^{2}(\mathbb {R})\), a linear canonical time shift operator \({\mathbf {T}_{s}^{A}}\) is given as
Linear canonical modulation: For a complex signal \(x(t) \in L^{2}(\mathbb {R})\), a linear canonical modulation operator \({\mathbf {M}_{u_{0}}^{A}}\) is given as
Convolution [25, 26]: For complex signals \(x_{1}(t), x_{2}(t) \in L^{2}(\mathbb {R})\), a convolution operator \(\circledast \) is given as
WignerVille distribution
The WVD plays a important role in timefrequency representation since it can provide good energy distribution and high resolution for nonstationary signal processing.
Definition 1. [1, 3] For complex signal \(x(t)\in L^{2}(\mathbb {R})\), the classical WVD of x(t) is defined as
which is FT of instantaneous autocorrelation function
Motivated by classical WVD and requirement of nonstationary signal processing, a series of novel WVD associated with LCT are proposed to process LFM signal and can be summarized in Table 2. As a matter of fact, above WVDs in LCT are obtained by using new transform kernel, new autocorrelation function, or other methods. As described in the Section 3, they need to improve performance in robust to noise and computational burden for signal processing. Besides, all of them do not fully utilize the characteristics of autocorrelation function of LFM signal and not remove the coupling relationship between time and time delay. Therefore, a newly defined WVD associated with LCT is first proposed in [21], which can remove the coupling and accumulate energy of LFM signal well in the timeLCF plane.
Method
This section will derive the WVDL from a new perspective and then study some useful properties in details. Based on these, a integration form of WVDL will be proposed to estimate parameters of LFM signal.
Definition of WVDL
It is well known that classical WVD in (9) is Fourier transform of autocorrelation function in (10). In order to obtain new WVDL, we define a new instantaneous autocorrelation function in LCT domain
Applying scaling FT to (11) along with scale time delay \(\frac {\tau }{b}\), it can be obtained
According to (11) and (12), a new WVDL can be defined.
Definition 2. [21] For complex signal \(x(t) \in L^{2}(\mathbb {R})\), the WignerVille distribution associated with LCT (WVDL) of x(t) is defined as
The \({WVDL}_{x}^{A}(t,u)\) displays the distribution of signal energy and can be finite support obviously over timeLCF plane, which can provide theoretical foundation for signal detection and estimation. Without loss of generality, assume that b>0, so b=b and they are not differentiated in the next sections. Particularly, when A=[0 1; −1 0], (13) will reduce to be classical WVD in (9).
It is worth pointing out that the existing other results of WVD in LCT domain [14–16, 18–20] can be regarded as the rotation or affine transform of the classical timefrequency plane. Similarly, there is a relationship between (13) and (9) [21]
In the practical engineering, it is finite for observation time to observe and process a system or a signal. Hence, for a LFM signal \(x(t)=e^{j\left (f_{0}t+\frac {k}{2}t^{2}\right)}\) with observation time T_{a}, its \({WVDL}_{x}^{A}(t,u)\) can be expressed as
where phase coefficients f_{0} and k are center frequency and modulation frequency rate respectively. From (15), a oblique line is shown in timeLCF plane, which represents the linear relationship between time and LCF. It is worth noting that a straight line paralleling to the time axis is obtained by (15) when \(\frac {a}{b}=k\), which is optimal and pivotal to energy gather and parameter estimation of LFM signal.
Properties of WVDL
Some interesting and basic properties of WVDL have been studied shown in Table 3 [21]. For the sake of completeness of the study on WVDL, there are other useful properties to be derived, which are helpful for analysis of cross term, the relationship of time width and bandwidth, filter design, and other feature analysis of signal. The properties and corresponding formulas are also summarized in Table 4.
(1) Nonlinearity: Let \({WVDL}_{x_{1}}^{A}(t,u), {WVDL}_{x_{2}}^{A}(t,u)\) be WVDLs of complex signal \(x_{1}(t), x_{2}(t) \in L^{2}(\mathbb {R})\) and x_{1}(t),x_{2}(t)≠0 respectively. If x(t)=x_{1}(t)+x_{2}(t), then \({WVDL}_{x}^{A}\) of x(t) is
Proof
According to the proposed definition of WVDL in (13), we have
From (17), the output includes two WVDLs of cross terms, which implies nonlinearity in (16) holds. □
(2) Linear canonical time shift: Let \({WVDL}_{x}^{A}(t,u)\) be WVDL of complex signal \(x(t)\in L^{2}(\mathbb {R})\), if \(\mathbf {T}_{s}^{A}[x(t)]=x(ts)\cdot e^{j\frac {a}{b}s\left (t\frac {s}{2}\right)}\), then
Proof
Based on time shift operator in (6) and definition of WVDL in (13), we have
This completes the proof. □
(3) Linear canonical modulation: Let \({WVDL}_{x}^{A}(t,u) \) be WVDL of complex signal \(x(t)\in L^{2}(\mathbb {R})\), if \(\mathbf {M}_{u_{0}}^{A}[x(t)]=x(t)\cdot e^{j\frac {u_{0}}{b}t}\), then
Proof
Based on modulation operator in (7) and definition of WVDL in (13), we have
Thus, linear canonical modulation property is proved. □
(4)Dilation: Let \({WVDL}_{x}^{A}(t,u) \) be WVDL of complex signal \(x(t)\in L^{2}(\mathbb {R})\), if \(\mathbf {D}_{t_{0}}[x(t)]=\frac {1}{t_{0}}x(t_{0} t)\), then
where \(A_{1}=\left [ t_{0}^{2}a\ \ b; \ \frac {c}{t_{0}^{2}} \ \ d\right ]\).
Proof
From dilation operator and definition of WVDL in (13), we obtain that
Let \(\frac {\tau }{t_{0}}=\tau ^{\prime }\), (23) can be written as
where \(A_{1}=\left [ t_{0}^{2}a\ \ b; \ \frac {c}{t_{0}^{2}} \ \ d\right ]\). This finishes the proof. □
(5) Reconstruction formula: Let \({WVDL}_{x}^{A}(t,u) \) be WVDL of complex signal \(x(t)\in L^{2}(\mathbb {R})\). If initial value x(0) of signal is known and x(0)≠0,b>0 then
Proof
The newly defined WVDL in (13) can be rewritten as
where \(\mathcal {F}\) is classical Fourier transform operator, and
Let \(t=\frac {\tau }{2}\), then τ=2t. (27) can be reduced
Further, let v=2t, then
Let t=v, we have
Thus, it completes the signal reconstruction. □
(6) Convolution: For complex signal \(x_{1}, x_2 \in L^{2}(\mathbb {R})\), then WVDL of \(x_{1} \circledast x_{2}\) is
Proof
First, we know
According to definition of WVDL, then
Let \(r=w+\frac {p}{2}, z=w\frac {p}{2}\) and τ=p+q, then (33) can be reduced as
which completes the proof. □
IWVDL method for LFM signal
LFM signal plays vital part in many signal processing scenarios like radar, communication, optical, and other fields. In this subsection, a integration form of WVDL (IWVDL) will be proposed for parameter estimation of LFM signal.
For monocomponent LFM signal,
its representation result can be obtained from (15)
The WVDL can gather energy of signal in the timeLCF plane, the maximum value of energy distribution is determined by \(k=\frac {a}{b}\). In order to enhance peak, we propose a integral way to WVDL along with time axis
Two phase parameters of LFM signal can be acquired simultaneously by the position of energy peak
In the observation time T_{a}, the multicomponent LFM signal is
where L is the number of component, C_{i},f_{i},k_{i} are the amplitude, center frequency and modulation frequency rate of the ith component, respectively. Applying WVDL to (39)
where
and as for the expression of cross terms, please see [21].
To enhance peak and suppress cross term, the integration along time axis is considered into WVDL
In the parameter search, cross term cannot be integrated actually since they contain t^{2}term in the exponential term and proposed method cannot match them.
Results and discussion
This section will dedicate to demonstrate the estimation performance of proposed method. The experiments for monocomponent and multicomponent LFM signal will be first performed. Then, error analysis, computation cost, and application in radar imaging field will be discussed.
Results
Experiment 1: Monocomponent LFM signal
In the observation time T_{a}=16s, monocomponent LFM signal in (35) with C=1,f=1, and k=−1 is shown in Fig. 1a, in which real part and imaginary part are blue solid line and red dotted line respectively. To indicate the characteristics of instantaneous frequency of signal in (35), an oblique line is reproduced by means of phase derivation in the timefrequency plane.
In order to display the feature of matched WVDL for LFM signal, Fig. 2 gives four WVDL results under four parameter matrices. Figure 2a can be viewed as classical WVD since A_{1}=[0 −1;1 0] is chosen, which gives the energy distribution in the classical timefrequency domain. Figure 2b–d are obtained respectively by WVDLs with A_{2}=[0.5 −1;1 0],A_{1}=[1 −1;1 0],A_{1}=[1.5 −1;1 0]. From Fig. 2c, proposed WVDL can obtain a straight line paralleling to the time axis, which is the optimal matched LCT domain. Figure 3 is the results by proposed IWVDL method, in which only Fig. 3c obtains a peak of LFM signal. Similar to other WVD in LCT domain [14–16, 18, 19], the results in the Fig. 2a, b, and d cannot acquire parameters of LFM signal directly in timeLCF plane since they still depend on time axis. Thus, Fig. 3a, b, and d after the integration cannot obtain energy peak of LFM signal. Figures 2c and 3c are able to obtain two phase coefficients of LFM signal simultaneously by proposed method.
Experiment 2: Multicomponent LFM signal
Without loss of generality, twocomponent LFM signal in (39) when L=2 is employed to validate proposed method. In the observation time T_{a}=16, the parameters of twocomponent LFM signal are amplitude C_{1}=C_{2}=1, phase coefficients f_{1}=1,f_{2}=−1, and k_{1}=−1,k_{2}=0.4. Figure 4a shows signal x(t) in time domain by real part and imaginary part.
Figure 5 is classical WVD over timefrequency plane, in which two intersecting lines only imply timefrequency distribution of two components and hardly obtain more special parametric information of signal. Figure 6 are the results by WVDL, in which the matched WVDL of x_{1} is shown and cross term can also not be ignored. Using characteristics of WVDL of LFM signal in timeLCF plane, IWVDL in Fig. 7 works well for suppressing cross term compared with Fig. 7. The parameters of twocomponent LFM signal can be estimated by peak search in the optimal and matched domain.
Discussion
Error analysis
In order to validate estimation performance of proposed method, we employ mean square error (MSE) to measured estimation error in different noise environment. The MSE of phase coefficients f and k can be given here [27]
and
where N_{t}rail is the number of simulation, \(\hat {f_{n}}\) and \(\hat {k_{n}}\) are the estimation values of phase coefficients f and k at the nth trail.
For existing WVDs in LCT domain [14–16, 18–20], there are some common problems for parameter estimation: (1) do not utilize the phase characteristics of autocorrelation function of LFM signal, (2) do not suppress cross term for multicomponent signal, and (3) need other method to further estimate parameters like least square method. Therefore, let us choose a common kind of WVD in LCT domain, the WDL in [15], to be compared to verify the better estimation performance of proposed method.
For LFM signal with additive white Gaussian noise, 100 Monte Carlo trails will be carried out under low signaltonoise rate (SNR) [ −15, −5] dB. The MSE of different LFM signals are shown in Fig. 8. Figure 8a is the result for monocomponent LFM signal, from which the method based on WDL displays larger error and our method will present higher accuracy for phase coefficients f and k in the [ −15, −5] dB. Besides, the estimation errors of multicomponent LFM signal are also measured and shown in Fig. 8b. In Fig. 8b, the estimation results based on WDL represent better accuracy in the lower SNR environment but the accuracy does not be improve when SNR increase. Proposed IWVDL method can obtain more accurate parameters when SNR ≥−12 dB and trend to be stable when SNR ≥−9 dB. Therefore, our proposed method is more robust against noise and has better estimation performance.
Computational cost
For a LFM signal with digital length N, the computation cost of classical WVD is O(N^{2}log_{2}N) based on fast FT. The computation cost of WDL is O(N^{3}) introduced by LCT kernel. The proposed IWVDL method contains free parameters of LCT, its computation includes autocorrelation function N, WVDL on autocorrelation function N^{2}. Assuming search times are M; therefore, the computational cost is O(MN^{3}). There are search procedures for other WVD in LCT domain; their computation become also more complex. For example, unified WVDs associated with LFM have nine or six free parameters, in which burden computation cost have to be faced.
Application
The inverse synthetic aperture radar (ISAR) imaging plays an important role for target recognition and classical in the military and civilian areas. The motion of observation target becomes more complex due to complex practical environment, especially the ship target over the sea. Its Doppler is no longer constant and shows timevarying by complex motion [28], which make rangeDoppler imaging algorithm based on FT difficult to obtain wellfocus ISAR image.
After range compression and motion compensation, the Doppler is generally modeled as LFM signal like (15) according to complex motion of rolling, roll, and yaw over the sea. Therefore, the azimuth echo in a range bin can be modeled as multicomponent LFM signal [29, 30]
where L is the number of scatterer in a range bin, and T_{a} is observation time. C_{i} is backward reflection coefficient, and a_{i1} and a_{i2} denote effective rotation velocity and accelerated velocity of scatterer i respectively.
Based on proposed IWVDL method, the parameters of each LFM signal in (45) can be estimated and cross term can be suppressed effectively. Figure 9 gives the ISAR imaging procedure based on proposed method. Associated with rangeinstantaneousDoppler imaging technique, the new ISAR imaging algorithm will be studied to obtain the highresolution ISAR image in our future work.
Conclusion
Jointing advantage of WVD and LCT in timefrequency plane, this paper derives a WVDL from a new autocorrelation function in LCT domain and investigate other useful properties. For LFM signal, this WVDL can remove coupling between time and time delay, which helps estimate parameter of LFM signal. Based on decoupling characteristics, an integration form of WVDL is proposed to enhance energy and suppress cross term. Then, two phase parameters can be estimated simultaneously to avoid error propagation. Moreover, the simulations are carried out by monocomponent and multicomponent LFM signal, which shows good ability on parameter estimation and suppression of cross term. Finally, the superior performance is verified by comparison and discussion of the estimation error and computational cost. The application on ISAR imaging field will be are studied in the future work.
Availability of data and materials
Please contact the authors for data requests.
Abbreviations
 WVD:

WignerVille distribution
 FT:

Fourier transform
 FRFT:

Fractional Fourier transform
 LCT:

Linear canonical transform
 UWDL:

Unified WVD in the LCT domain
 LCF:

Linear canonical frequency
 WVDL:

WignerVille distribution associated with linear canonical transform
 LFM:

Linear frequency modulation
References
K. Gröchenig, Foundations of TimeFrequency Analysis (Birkhäuser, Boston, Mass, USA, 2001).
D. Dragoman, Applications of the Wigner distribution function in signal processing. EURASIP J. Adv. Signal Process.2005:, 264967 (2005).
L. Debnath, B. V. Shankara, N. Rao, On new two dimensional WignerVille nonlinear integral transforms and their basic properties. Integr. Transf. Spec. F.21(3), 165–174 (2010).
C. Y. Mei, A. Z. Sha’ameri, B. Boashash, Efficient phase estimation for the classification of digitally phase modulated signals using the crossWVD: a performance evaluation and comparison with the Stransform. EURASIP J. Adv. Signal Process.2012:, 65 (2012).
Y. S. Wu, X. K. Li, Elimination of crossterms in the WignerVille distribution of multicomponent LFM signals. IET Signal Process.11(6), 657–662 (2017).
H. N. Su, J. M. Pan, Q. L. Bao, Z. P. Chen, Parameter estimation of linear frequency modulated signals based on a WignerVille distribution complexvalued convolutional neural network. J. Appl. Rem. Sens.14(3), 036512 (2020).
R. Tao, B. Li, Y. Wang, G. K. Aggrey, On sampling of bandlimited signals associated with the linear canonical transform. IEEE Trans. Signal Process.56(11), 5454–5464 (2008).
B. Z. Li, T. Z. Xu, Linear canonical transform and application (Science Press, China, 2013).
Y. Sun, B. Z. Li, Sliding discrete linear canonical transform. IEEE Trans. Signal Process.67(7), 4553–4563 (2018).
N. Goel, K. Singh, R. Saxena, A. K. Singh, Multiplicative filtering in the linear canonical transform domain. IET Signal Process.10(2), 173–181 (2016).
X. Huang, L. R. Zhang, S. Y. Li, Y. H. Zhao, Radar high speed small target detection based on keystone transform and linear canonical transform. Digit. Signal Process.82:, 203–215 (2018).
J. Shi, X. Liu, X. J. Fang, X. J. Sha, W. Xiang, Q. Y. Zhang, Linear canonical matched filter: theory, design, and applications. IEEE Trans. Signal Process.66(24), 6404–6417 (2018).
Y. N. Zhang, B. Z. Li, N. Goel, S. Gabarda, Quantitative SNR analysis of QFM signals in the LPFT domain with Gaussian windows. Sci. China Inform. Sci.62(2), UNSP 15 (2019).
S. C. Pei, J. J. Ding, Relations between fractional operations and timefrequency distributions, and their applications. IEEE Trans. Signal Process.49(1), 1638–1655 (2001).
R. F. Bai, B. Z. Li, Q. Y. Cheng, WignerVille distribution associated with the linear canonical transform. J. Appl. Math.2012:, 740161 (2012).
D. Y. Wei, Y. M. Li, Linear canonical Wigner distribution and its application. Optik. 125(1), 89–92 (2014).
Y. E. Song, X. Y. Zhang, C. H. Shang, H. X. Bu, X. Y. Wang, The WignerVille distribution based on the linear canonical transform and its applications for QFM signal parameters estimation. J. Appl. Math.2014:, 516457 (2014).
Z. C. Zhang, M. K. Luo, New integral transforms for generalizing the Wigner distribution and ambiguity function. IEEE Signal Process. Lett.22:, 460–464 (2015).
Z. C. Zhang, Unified WignerVille distribution and ambiguity function in the linear canonical transform domain. Signal Process.114:, 45–60 (2015).
Z. C. Zhang, New Wigner distribution and ambiguity function based on the generalized time shift in the linear canonical transform domain. Signal Process.118:, 51–61 (2016).
Z. C. Zhang, Novel Wigner distribution and ambiguity function associated with the linear canonical transform. Optik. 127(12), 4995–5012 (2016).
D. Urynbassarova, B. Z. Li, R. Tao, Convolution and correlation theorems for WignerVille distribution associated with the offset linear canonical transform. Optik. 157:, 455–466 (2018).
L. Y. Zheng, D. Shi, J. Zhang, CAFFrFT: a centeraffinefilter with fractional Fourier transform to reduce the crossterms of Wigner distribution. Signal Process.94:, 330–338 (2014).
Z. Z. Guan, G. K. Xia, Q. Meng, Signal and linear systems (Higher Education Press, Beijing, 2004).
B. Deng, R. Tao, Y. Wang, Comments on a convolution and product theorem for the linear canonical transform. IEEE Signal Process. Lett.17(6), 615–616 (2010).
D. Y. Wei, Y. M. Li, Convolution and multichannel sampling for the offset linear canonical transform and their applications. IEEE Trans. Signal Process.67(23), 6009–6024 (2019).
M. Huber, L. Czeslaw, D. Igor, Estimating the instantaneous frequency of linear and nonlinear frequency modulated radar signalsa comparative study. Sensors. 21(8), 2840 (2021).
M. D. Xing, R. Wu, Y. C. Li, Z. Bao, New ISAR imaging algorithm based on modified WignerVille distribution. IET Radar Sonar Navig. 3(1), 70–80 (2008).
Y. Wang, Y. Lin, ISAR imaging of nonuniformly rotating target via rangeinstantaneousDopplerderivatives algorithm. IEEE J. Sel Top. Appl. Earth Obs. Remote Sens.7(1), 167–176 (2014).
J. B. Zheng, H. Liu, Q. H. Liu, Parameterized centroid frequencychirp rate distribution for LFM signal analysis and mechanisms of constant delay introduction. IEEE Trans. Signal Process.65(24), 6435–6447 (2017).
Acknowledgements
The author is very thankful to all colleagues and reviewers for their help and useful suggestions on this paper.
Funding
This work was supported by the National Natural Science Foundation of China [No. 61671063] and China Scholarship Council [No. 201906030148].
Author information
Affiliations
Contributions
Authors’ contributions
HCX contributed to propose newly and specially defined WVDL and derive its useful properties. Besides, HCX contributed to simulation and manuscript by softwares. BZL contributed to the conception of new WVDL and review. Moreover, BZL contributed to the funding support. The authors read and approved the final manuscript.
Authors’ information
HongCai Xin was born in Handan, China, in 1991. She received the B.S. degree from Hebei Normal University, Shijiazhuang, China, in 2015. She is currently working towards the Ph.D. degree in Beijing Institute of Technology, Beijing, China. Her research interests include the theory and applications of fractional Fourier transform and linear canonical transform, inverse synthetic aperture radar (ISAR) and interferometric ISAR (InISAR), and timefrequency analysis.
BingZhao Li was born in 1975. He received the B.S. degree from Shandong Normal University in 1998, and the M.S. and Ph.D. degrees from Beijing Institute of Technology, in 2001 and 2007, respectively. He is currently a Professor with the School of Mathematics and Statistics, Beijing Institute of Technology, Beijing, China. He was a recipient of National Excellent Doctoral Dissertation Award Nomination and Henry Fok Education Foundation Young Teacher Award in 2010, and also supported by the New Century Excellent Talents in University in 2012. He is currently the Vice Dean of the School of Mathematics and Statistics. His current research interests include the theory and applications of fractional Fourier transform, linear canonical transform, and fractional calculus. He has published one book and more than 40 peerreviewed journal articles.
Corresponding author
Ethics declarations
Consent for publication
This research does not contain any individual person’s data in any form (including individual details, images, or videos).
Competing interests
The authors declare that they have no competing interests.
Additional information
Publisher’s Note
Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Rights and permissions
Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/.
About this article
Cite this article
Xin, HC., Li, BZ. On a new WignerVille distribution associated with linear canonical transform. EURASIP J. Adv. Signal Process. 2021, 56 (2021). https://doi.org/10.1186/s13634021007533
Received:
Accepted:
Published:
DOI: https://doi.org/10.1186/s13634021007533
Keywords
 Linear canonical transform
 WignerVille distribution
 Timefrequency analysis
 Parameter estimation