1 LV Distribution, Performance and Applications Presented by: Bi Guoan School of Electrical and Electronic Engineering Nanyang Technological University.

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Presentation transcript:

1 LV Distribution, Performance and Applications Presented by: Bi Guoan School of Electrical and Electronic Engineering Nanyang Technological University Singapore

2 Outline  Introduction  Lv distribution (LVD) –Definition and properties –Performances  Application –SAR image processing  Conclusion

Introduction  Most real signals contain frequencies varying with time – known as non-stationary or time-varying  Fourier transform tells us the frequencies in the signals, but not how they change with time.  Time frequency signal analysis has been useful to truthfully reveal the useful information matching with our observations, Example.Example. 3

Introduction  A time–frequency distribution should have the following desirable features: −High signal concentration for accurate analysis and interpretation. −No cross-term to avoid confusing components duo to the imperfection of the processing methods 4 −Desirable mathematical properties ensure such methods beneficial to real-life applications. −Lower computational complexity to ensure the time needed to process the signal for real-time implementations.

Introduction  Well known time frequency representations (TFRs): −STFT (Gabor transform): simple with low resolution limited to uncertainty principle (TFR). −Local Polynomial periodogram (LPP) : requires much more computation for estimation of polynomial coefficient (TFR) −WVD or smoothed pseudo WVD : providing best signal concentration, but suffering from the cross-term for multi- component signals 5 −Fractional Fourier transform: a rotation operation on TFRs to find the best signal concentration −Wavelet transform: no direct physical meaning from the results

6 Introduction  The frequencies of time varying signals may change in various ways.  Within a short time period, we assume the frequencies are changing linearly −Linear frequency modulated (LFM) signal: −Two types of signal representations: Time-frequency representations (TFRs) Frequency chirp rate representations (FCRs) centroid frequency chirp rate

Introduction 7 −Reduced resolution and cross-terms −Trade-off between auto- terms and cross-terms −Better resolution than STFT −Some small cross-terms −No cross-term, −poor resolution −High resolution −Heavy cross-terms

Introduction  For critical environments, such as low SNR and multiple signal components, most of these methods are not usable.  Other suitable methods are required to obtain a balanced performance among a few contradictory requirements −High signal concentration with strong noise environment −Low cross-terms among different components −High signal resolution and −Low computation complexity  LV distribution (LVD) is a new algorithm achieving the above requirements 8

9 Outline  Introduction  Lv distribution (LVD) –Definition and properties –Performances  Application –SAR image processing  Conclusion

10 Lv distribution (LVD)  The LVD* –Combines the desirable properties of linear and bilinear methods for dealing with LFM signals –Provides peaks for each LFM components in the FCR domain –Main merits: High resolution/concentration Asymptotic linear (very small cross-terms can be ignored) Reasonable computational complexity *X. Lv, G. Bi, C. Wan, and M. Xing, Lv's distribution: Principle, implementation, properties, and performance, IEEE Transactions on Signal Processing, vol. 59, no. 8, pp , Aug

11 Lv distribution (LVD)  Definition : a parametric symmetric instantaneous autocorrelation function (PSIAF) of the input signal x(t) :  A scaling operator  of a phase function G with respect to (t,  ) as : constant time-delay cross- terms h : a scaling factor t and  are coupled together, leading to cross term effects auto-terms

12 Lv distribution (LVD)  Definition of the LVD −Perform the scaling operation  on the PSIAF and obtain −Take the 2-D FT of the previous equation with respect to  and t n auto-term cross-term t and  are decoupled

13 Lv distribution (LVD)  Definition of the LVD For a multi-component LFM signal, the LVD is asymptotic linear as The LVD has: three components; very little cross-terms; high resolution.

14 Lv distribution (LVD)  Properties of the LVD –Asymptotic linear: –Frequency and chirp rate shift: if we have –Resolution: –Others: scaling, translation, convolution, etc.

15 Lv distribution (LVD)  Performance of the LVD –Representation comparison LVD RWT RAT FrFT LVD: no obvious cross-terms high concentration

16 Lv distribution (LVD)  Performance of the LVD –Resolution Three LFM components with differences in centroid frequencies by 2 Hz and in chirp rates by 2 Hz/s ---- only the LVD can distinguish them LVD: most narrow main-lobe width; highest resolution. ?

17 Lv distribution (LVD)  Performance of the LVD –Representation errors: mean square error (MSE) MSEs of the LVD are lowest, and approach to the Cramer-Rao lower bounds (CRLBs) at lowest SNR

18 Lv distribution (LVD)  Performance of the LVD –LFM signal Detection: The threshold in LVD is and theoretical detection probability is : false alarm probability : cumulative distribution function of a standard normal distribution

19 Lv distribution (LVD)  Performance of the LVD –LFM signal Detection: Input sample length N = 512

20 Lv distribution (LVD)  Performance of the LVD –Computational complexity They are all in the same order of, indicating that LVD provides better performance without introducing more computational complexity. N s : input length

21 Outline  Introduction  Lv distribution (LVD) –Definition, properties –Performances  Application –SAR image processing  Conclusion

22 Synthetic Aperture Radar (SAR) Fundermental swath height synthetic aperture

Time-Frequency Based Moving Target Imaging After clutter suppression, the phase history of each range cell containing one or multiple moving targets can be modeled as: is the amplitude is the Doppler centroid frequency is the Doppler chirp rate is the target number Due to the target velocity in along- and cross-track resulting in Doppler frequency shift and Doppler frequency modulation, respectively, the moving target image will be shifted and unfocused. The moving target phase history has the linear frequency modulation (LFM) form. Time-frequency analysis is more suitable. Under the relationship between the centroid frequency and chirp rate and the velocity in along- and cross-track, the motion parameters can be expressed by time- frequency distribution (TFD). –L. Yang, G. Bi, M. Xing and L. Zhang, “Airborne SAR moving target signatures and imagery based on LVD,” To appear in IEEE Transactions on Geoscience and Remote Sensing, 2015.

Fig.1 (a) Point Moving Targets Simulation (MT1-MT5 are moving targets; ST1-ST2 are stationary targets; MT1-MT3 are located in the same range cell, and MT4- MT5 are located in the other same range cell) (Green rectangles are the shifted position of the moving targets; red crosses are the true position of the moving targets) (Fig. 1(a) is the simulation result; Fig. 1(b) is the defocused moving targets image of MT4; Fig. 1(c) is the refocused moving targets image of MT4) Since the velocity of the moving target in cross-track will induce the position shift in azimuth direction, and the velocity in along-track will cause defocusing in azimuth direction, therefore, by applying the LVD for the SAR moving target imaging, the targets are relocated to the true (original) position and refocused to obtain the true SAR moving targets. Although there are more than one target are located in the two separated range cell, the SAR moving targets are focused into high quality. Fig.1 (c) Fig.1 (b)

Fig.1 (a) Fig. 1(a) is the SAR image with the moving targets by the raw SAR data; Fig. 1(b) is the defocused moving targets image of T6; Fig. 1(c) is the refocused moving targets image of T6; Fig.1 (b) Fig.1 (c)

Fig.1 (b) Fig.1 (c)

27 Thank you!