Detection of Low-observable Maneuvering Target Using High-order Generalized Lv’s Distribution
Xiaolong Chen, Xiuyou Li, Yunlong Dong, Yong Huang, Jian Guan, You He Marine Target Detection Research Group, Naval Aeronautical and Astronautical University, Yantai, Shandong P.R. China Email:
[email protected]
Overview 1. Introduction Difficulty of low-observable maneuvering target detection Research situation Signal model for long-time observation
2. Principle of HGLVD-based detection method Definition Long-time coherent integration Detection algorithm
3. Experiments (application of marine target detection) Micro-Doppler signature Experiments with CSIR data
4. Conclusions
Marine Target Detection Research Group, NAAU
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2016-04-27
Overview 1. Introduction Difficulty of low-observable maneuvering target detection Research situation Signal model for long-time observation
2. Principle of HGLVD-based detection method Definition Long-time coherent integration Detection algorithm
3. Experiments (application of marine target detection) Micro-Doppler signature Experiments with CSIR data
4. Conclusions
Marine Target Detection Research Group, NAAU
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1.1 Difficulty 1)Low-observable target detection
Small size
Stealth
Far-range
+
Complex environment
Lowobservable target 1
High-speed or highly mobile
Amplitude Normalized Amplitude
浮海浮海浮浮
Target
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0.6
0.4
0.2
0
100
200
300
400
500
!Effective solution: Clutter suppression; Accumulate target’s energy to improve SCR/SNR. Marine Target Detection Research Group, NAAU
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Samples Range
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1000
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1.1 Difficulty 2)Clutter Clutter is one of the most important factors for low-observable target detection. For example, strong sea clutter (sea spikes) usually show nonhomogeneous, nonstationary, and time-varying properties, which would degrade the detection performance of radar detectors. Target Sea clutter Target Sea clutter
14
Sea spikes
Frequency domain 幅幅
Time domain
海海海 Doppler spread 海海海(无海海海)
12 10 8 6 4 2 -100
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-50
0 50 频频 (Hz)
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100
150
1.1 Difficulty
Phased array radar, MIMO radar Multiple beams controlled by DBF technology Electronic beam scanning Cover wider space arbitrarily The dwell time is enough for long-time integration
Marine Target Detection Research Group, NAAU
With the development of digital phased array technology, it is possible to detect low-observable target via longtime integration, which is an effective way to improve SCR.
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1.2 Research situation Across range unit (ARU): range migration
—Both amplitude and Doppler information
Envelope correlation;
Poor performance
Keystone transform (KT);
in low SNR/SCR
Radon-Fourier transform (RFT)
environment; Doppler ambiguity;
Frequency
Coherent integration technique
Problems:
DFM
Cannot correct
ARU
range curvature
Range
Doppler frequency migration (DFM): Chirp-Fourier transform;
Limited pulses for
Chirplet transform;
integration
Fractional Fourier transform (FRFT)
We need a method to deal with ARU, range curvature, and DFM effects for weak maneuvering target. Marine Target Detection Research Group, NAAU
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1.2 Research situation Long-time coherent integration
Radon-Fourier transform (RFT) : Generalized RFT (GRFT) …….
Marine Target Detection Research Group, NAAU
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1.2 Research situation Radon-fractional Fourier transform (RFRFT)、Radon-Linear Canonical Transform (RLCT) Radon-fractional ambiguity function (RFRAF)、Radon-Linear Canonical ambiguity function (RLCAF)
MTD: SMTD = ∫ sPC (t , tm )exp( − j2πf dtm )dtm
RFT: SRFT = ∫ sPC [ 2(r0 − v0tm ) / c, tm ] exp( − j2πf dtm )dtm
α=π/2
α=π/2 FRFT: S RFRFT = ∫ sPC (t , tm ) Kα (tm , u )dtm
2 RFRFT: SRFRFT = ∫ sPC 2(r0 − v0tm − astm / 2) / c, tm Kα (tm , u )dtm
One rangebin
Marine Target Detection Research Group, NAAU
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1.3 Signal model for long-time observation After demodulation and pulse compression Across range unit (ARU) effect
sPC ( t , tm ) = Ar sinc B ( t − τ ) exp ( − j2πf cτ )
Fast time
Slow-time
τ = 2rs (tm ) / c
!The target’s envelope has been shifted away from its original position due to its motion.
For a maneuvering target, its Doppler can be approximated as 2 drs (tm ) rs → ( r0 , v0 , as , tm ) f 0 + µs tm fd = , , fd = 2 ( , , , , ) r → r v a g t λ dtm f 0 + µs tm + g s tm / 2 s 0 0 s s m
Doppler frequency migration (DFM)
!The acceleration and jerk will have an impact on the range curvature and Doppler spread. 200
150
Chen Xiaolong, et al. Maneuvering target detection via Radon-fractional Fourier transform-based long-time coherent integration. IEEE TSP, 2014, 62(4): 939-953.
Doppler 海海海海
100
Chen Xiaolong, et al. Radon-fractional ambiguity functionbased detection method of low-observable maneuvering target. IEEE TAES, 2015, 51(2): 815-833.
50
Clutter and noise 海海海海海海 0
-50
0
0.5
1
1.5
2
2.5
3
3.5
4
4.5
Chen Xiaolong, et al. Radon-linear canonical ambiguity function-based detection and estimation method for marine target with micromotion. IEEE TGRS, 2015, 53(4): 2225-2240.
t (s)
Marine Target Detection Research Group, NAAU
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2016-04-27
1.3 Signal model for long-time observation After demodulation and pulse compression Across range unit (ARU) effect
sPC ( t , tm ) = Ar sinc B ( t − τ ) exp ( − j2πf cτ )
Fast time
Slow-time
τ = 2rs (tm ) / c
!The target’s envelope has been shifted away from its original position due to its motion.
For a maneuvering target, its Doppler can be approximated as Doppler frequency migration (DFM)
2 drs (tm ) rs → ( r0 , v0 , as , tm ) f 0 + µs tm fd = , , fd = 2 ( , , , , ) r → r v a g t λ dtm f 0 + µs tm + g s tm / 2 s 0 0 s s m
!The acceleration and jerk will have an impact on the range curvature and Doppler spread.
In this paper, a novel long-time coherent integration method (High-order Generalized Lv’s Distribution, HGLVD) is proposed to achieve better detection performance without requiring more computational cost. Marine Target Detection Research Group, NAAU
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2016-04-27
Overview 1. Introduction Difficulty of low-observable maneuvering target detection Research situation Signal model for long-time observation
2. Principle of HGLVD-based detection method Definition Long-time coherent integration Detection algorithm
3. Experiments (application of marine target detection) Micro-Doppler signature Experiments with CSIR data
4. Conclusions
Marine Target Detection Research Group, NAAU
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2016-04-27
2.1 Definition of HGLVD Time delay Slow-time High-order motion τ τ Pf (tm , rs ) = f tm + 0 , rs f * tm − 0 , rs 2 2
Phase differentiation (PD) calculation τ +b * τ +b R f (tm ,τ , rs ) = f tm + , rs f tm − , rs 2 2
Radon instantaneous auto-correlation function (RIAF)
t
n ,τ , rs Scaling processing S R f (tm ,τ , rs ) = R f q(τ + b)
2-D RFT operator Marine Target Detection Research Group, NAAU
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2.2 Long-time coherent integration f (tm ) = exp j ( a0 + a1tm + a2 tm2 + a3tm3 ) τ τ Pf (tm , rs ) = f tm + 0 , rs f * tm − 0 , rs 2 2
Phase differentiation (PD) calculation
Pf (tm , rs ) = exp j ( a1τ 0 + a3τ 03 / 4 + 2a2τ 0tm + 3a3τ 0tm2 )
τ +b * τ +b R f (tm ,τ , rs ) = f tm + , rs f tm − , rs 2 2
Radon instantaneous auto-correlation function (RIAF)
t
R f [τ , Pf (tm , rs )] = exp [2 ja2τ 0 (τ + b) + 6 ja3τ 0 (τ + b)tm ]
n S R f (tm ,τ , rs ) = R f ,τ , rs q ( + b) τ
Scaling processing 2-D RFT operator
R f (tn ,τ , rs ) = exp [ 2 ja2τ 0 (τ + b) + j6a3τ 0tn / q ]
+∞
H R ( g , a, rs ) = Rτ ( Rtn ) = ∫−∞ =e
The signal will appear as a peak in the (a,g) domain Marine Target Detection Research Group, NAAU
∫
+∞
−∞
R f (tn ,τ , rs )e − j(g + a ) tn dtn dτ
δ ( a − 2a2τ 0 ) δ ( g − 6τ 0 a3 / q )
j2 a2τ 0 b
6 2 ( a, g ) = 2a2τ 0 , a3τ 0 = 2πµτ 0 , kτ 0 q q 14
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2.3 Detection algorithm Radar returns after demodulation and pulse compression
Phase differentiation (PD) calculation Parameters initialization
Radon instantaneous auto-correlation function (RIAF)
HGLVD-based long-time coherent integration
Scaling processing 2-D RFT operator
Form the detection statistic and carry out the CFAR detection
Motion Parameters estimation
Marine Target Detection Research Group, NAAU
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2016-04-27
Overview 1. Introduction Difficulty of low-observable maneuvering target detection Research situation Signal model for long-time observation
2. Principle of HGLVD-based detection method Definition Long-time coherent integration Detection algorithm
3. Experiments (application of marine target detection) Micro-Doppler signature Experiments with CSIR data
4. Conclusions
Marine Target Detection Research Group, NAAU
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3.1 Micro-Doppler signature Under high oceanic conditions, or due to the pushing and control effects caused by propeller, engine, and rudder, the attitude of target may vary with the fluctuation of sea surface, which induces the effect of power modulation on radar echo. The Doppler exhibits time-varying and nonstationary properties, which is periodically frequency modulated.
Marine Target Detection Research Group, NAAU
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3.1 Micro-Doppler signature
① Chen Xiaolong, et al. Effective coherent integration method for marine target with micromotion via phase differentiation and radon-Lvs distribution. IET RSN (special issue: m-D), 2015, 9(9): 1284-1295.
② Chen Xiaolong, et al. Sea clutter suppression and micromotion marine target detection via Radonlinear canonical ambiguity function. IET RSN, 2015, 9(6): 622-631.
③ Chen Xiaolong, et al. Radon-linear canonical ambiguity function-based detection and estimation method for marine target with micromotion. IEEE TGRS, 2015, 53(4): 2225-2240.
④ Chen Xiaolong, et al. Detection of a low observable sea-surface target with micromotion via the Radon-linear canonical transform. IEEE GRSL, 2014, 11(7): 1225-1229. Marine Target Detection Research Group, NAAU
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3.2 Experiments with CSIR data The measurement trial was conducted with the Fynmeet dynamic RCS measurement facility at the over-berg test range (OTB) in 2006. Sea clutter at grazing angles 0.501– 0.56° were recorded. The TFA17_014 dataset was chosen and the cooperative marine target named as WaveRider rigid inflatable boat (RIB) was deployed for the purpose of recording reflectivity measurement dataset.
Experiments Configurations
Marine Target Detection Research Group, NAAU
Plan overview of deployment site of the Fynmeet radar at OTB 19
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3.2 Experiments with CSIR data
Range profiles of sea clutter with the WaveRider RIB
High Doppler resolution spectrogram of targetGroup, range bin 18 Marine Target Detection Research NAAU
Range migration and GPS trajectory of the target
High Doppler resolution spectrogram of target range 20 bin 20 2016-04-27
3.2 Experiments with CSIR data 1
1
RFT GRFT
Target energy
0.8
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0.6 Sea clutter
0.5 0.4 0.3
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0.1
0.1
-200
-100 0 100 Frequency (Hz)
200
300
RFT and GRFT outputs (TFA17_014 dataset, Tn=5.12 s, 2048 pulses)
s
0.6
0.2
-300
v (m/s)=-0.54 0 a (m/s2)=0.36 s g (m/s3)=0.046 s r (m)=-29.33
Target
0.9
PD-RLVD outpurs
Outputs
0.9
-200
-100
0 Chirp rate (Hz/s)
100
200
HGLVD outputs (TFA17_014 dataset, Tn=5.12 s, 2048 pulses)
HGLVD
Comparisons of detection and computational burden performances (Pfa = 10−4)
Marine Target Detection Research Group, NAAU
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Applications in radar signal processing
Wideband radar (High range resolution)
① ⑤ Ability to suppress clutter and noise
④
RFRFT RLCT RFRAF RLCAF HGLVD
Low observable target detection (Far range、stealth target)
②
③
High-speed or highly mobile target
Digital phases array radar
clutter
Xiaolong Chen, et al. An effective coherent integration method for marine target with micromotion via PD-RLVD, Accepted by IETGroup, RadarNAAU sonar and Navigation, special issue for micro-Doppler, 2015. Marine Target Detection Research 22 2016-04-27
Overview 1. Introduction Difficulty of low-observable maneuvering target detection Research situation Signal model for long-time observation
2. Principle of HGLVD-based detection method Definition Long-time coherent integration Detection algorithm
3. Experiments (application of marine target detection) Micro-Doppler signature Experiments with CSIR data
4. Conclusions
Marine Target Detection Research Group, NAAU
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4. Conclusions A novel detection method for low-observable target is proposed via HGLVD, which not only achieves long-time coherent integration but also directly represents the target’s signal in the 2-D CRCC domain. It is proved that HGLVD has great application potentials for target with high-order motion without introducing any nonphysical attributes such as order or rotation angle. The performance is validated by experiments using Xband CSIR data. Future work will focus on the applications and its fast calculations.
Marine Target Detection Research Group, NAAU
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2016-04-27
Xiaolong Chen Marine Target Detection Research Group, Naval Aeronautical and Astronautical University Email:
[email protected]