MITSUBISHI ELECTRIC RESEARCH LABORATORIES Cambridge, Massachusetts High resolution SAR imaging using random pulse timing Dehong Liu Joint work with Petros Boufounos. IGARSS’ 2011 Vancouver, CANADA MITSUBISHI ELECTRIC RESEARCH LABORATORIES Outline • Overview of synthetic aperture radar (SAR) • Compressive sensing (CS) and random pulse timing • Iterative reconstruction algorithm • Imaging results with synthetic data • Conclusion and future work 2 MITSUBISHI ELECTRIC RESEARCH LABORATORIES Overview of SAR 3 MITSUBISHI ELECTRIC RESEARCH LABORATORIES 4 Synthetic Aperture Radar (SAR) v Reflection duration depends on range length. azimuth azimuth Ground Range MITSUBISHI ELECTRIC RESEARCH LABORATORIES 5 Strip-map SAR: uniform pulsing v azimuth azimuth Ground Range MITSUBISHI ELECTRIC RESEARCH LABORATORIES Data acquisition and image formation • SAR acquisition follows linear model y = x, where y: Received Data, x: Ground reflectivity, : Acquisition function determined by SAR parameters, for example, pulse shape, PRF, SAR platform trajectory, etc. • Image formation: determine x given – Range Doppler Algorithm – Chirp Scaling Algorithm • Specific to Chirp Pulses y and . 6 MITSUBISHI ELECTRIC RESEARCH LABORATORIES 7 SAR imaging resolution • Range resolution – Determined by pulse frequency bandwidth • Azimuth resolution Range – Determined by Doppler bandwidth – Requiring high Pulse Repetition Frequency (PRF) azimuth MITSUBISHI ELECTRIC RESEARCH LABORATORIES 8 Trade-off for uniform pulse timing T T T T Reflection Reflection T Reflection Reflection T overlapping T Reflection T Reflection Low azimuth resolution, large range. Reflection High azimuth resolution, small range. Reflection High azimuth resolution, large range ? missing • Tradeoff between azimuth resolution and range length – Reflection duration depends on range length – Increasing PRF reduces the range length we can image – High azimuth resolution means small range length. MITSUBISHI ELECTRIC RESEARCH LABORATORIES 9 Ground coverage at high PRF azimuth range • Issue: missing data always in the same range interval – Produces black spots in the image – High resolution means small range coverage • Solution: Motivated by compressive sensing, we propose random pulse timing scheme for high azimuth resolution imaging. MITSUBISHI ELECTRIC RESEARCH LABORATORIES Compressive sensing and random pulse timing 10 MITSUBISHI ELECTRIC RESEARCH LABORATORIES Compressive sensing vs. Nyquist sampling • Nyquist / Shannon sampling theory – Sample at twice the signal bandwidth • Compressive sensing – Sparse / compressible signal – Sub-Nyquist sampling rate – Reconstruct using the sparsity model 11 MITSUBISHI ELECTRIC RESEARCH LABORATORIES 12 Compressive sensing and reconstruction • CS measurement x W Φ sparse signal measurements Non-zeroes • Reconstruction x arg min x • • • 1 2 y x 2 2 W 1 x 1 Signal model: Provides prior information; allows undersampling; Randomness: Provides robustness/stability; Non-linear reconstruction: Incorporates information through computation. MITSUBISHI ELECTRIC RESEARCH LABORATORIES Connection between CS and SAR imaging SAR imaging CS Data acquisition Random projection measurements y x Radar echo CS measurements Ground reflectivity Sparse signal Acquisition function determined by SAR parameters Random projection matrix Image formation Sparse signal reconstruction y=x x | y, Question: Can we apply compressive sensing to SAR imaging? 13 MITSUBISHI ELECTRIC RESEARCH LABORATORIES 14 Random pulse timing Randomized timing mixes missing data Randomized pulsing interval azimuth range MITSUBISHI ELECTRIC RESEARCH LABORATORIES Iterative reconstruction algorithm 15 MITSUBISHI ELECTRIC RESEARCH LABORATORIES Iterative reconstruction algorithm Note: Fast computation of and H always speeds up the algorithm. 16 MITSUBISHI ELECTRIC RESEARCH LABORATORIES Efficient computation 17 Chirp Scaling Algorithm y Azimuth FFT Fa Chirp Scaling (differential RCMC) S-1 Range FFT Fr x F 1 a H a 1 1 1 H P Fr R B Pr Fr S Fa PrH Bulk RCMC, RC, SRC B-1 R-1 Range IFFT Fr-1 Azimuth Compression/ Phase Correction PaH Azimuth IFFT Fa-1 Computation of follows reverse path Computation as efficient as CSA 1 H 1 1 1 H 1 H xˆ Fa Pa Fr R B Pr Fr S Fa y y 1 H x MITSUBISHI ELECTRIC RESEARCH LABORATORIES Imaging results with synthetic data 18 MITSUBISHI ELECTRIC RESEARCH LABORATORIES Experiment w/ synthetic data • SAR parameters: RADARSAT-1 • Ground reflectivity: Complex valued image of Vancouver area • Quasi-random pulsing: Oversample 6 times in azimuth, and randomly select half samples to transmit pulses, resulting 3 times effective azimuth oversampling. • Randomization ensures missing data well distributed 19 MITSUBISHIRadar ELECTRIC RESEARCH LABORATORIES data acquisition Ground Forward process 20 Radar Raw Data Radar Image CSA imaging result with full uniformly-sampled data 0.1 0.09 2000 Standard Algorithm 0 0.08 0.07 4000 0.06 6000 2000 0.05 0.04 8000 0.03 4000 0.02 Azimuth 10000 0.01 6000 Classic Pulsing 12000 low PRF 8000 200 400 600 800 1000 0 Image with low azimuth resolution Conjugate gradient imaging result with random pulsing (L2 constraint) 0.1 10000 0.09 2000 12000 0 200 400 600 800 Iterative Algorithm 1000 Range Simulated Ground Reflectivity (high-resolution) 0.08 0.07 4000 0.06 6000 0.05 0.04 8000 0.03 0.02 10000 0.01 12000 Random Pulsing high PRF + missing data 200 400 600 800 1000 0 Image with high azimuth resolution Random pulsing, High PRF, Large Doppler Bandwidth Uniform pulsing, Small PRF, Small Doppler Bandwidth True Ground Reflectivity MITSUBISHI ELECTRIC RESEARCH LABORATORIES Zoom-in imaging results 21 Random pulsing, High PRF, Large Doppler Bandwidth Uniform pulsing, Small PRF, Small Doppler Bandwidth True Ground Reflectivity MITSUBISHI ELECTRIC RESEARCH LABORATORIES Zoom-in imaging results 22 MITSUBISHI ELECTRIC RESEARCH LABORATORIES Conclusion and future work 23 MITSUBISHI ELECTRIC RESEARCH LABORATORIES Conclusion • Proposed random pulse timing scheme with high average PRF for high resolution SAR imaging. • Utilized iterative non-linear CS reconstruction method to reconstruct SAR image. • Achieved high azimuth resolution imaging results without losing range coverage. Future work • Noise and nadir echo interference issues. • Computational speed. 24