Abstract

Bistatic sonar or multistatic sonar system can collect more scattering information of targets than a monostatic sonar system. In this paper, sparse learning via iterative minimization method (SLIM) is introduced to distinguish wave components for time-domain (TD) back-propagation (BP) inverse scattering imaging improvement. Unlike the prevailing high central frequency (>100 kHz) and wideband imaging sonar systems, a relatively low-frequency band (1–10 kHz) is considered here. Due to the low sidelobe output of SLIM, the investigated object’s surface in TD-BP image is much clearer in an ideal two-dimensional free field case. Furthermore, when the environmental information is known, this sparse reconstruction-based channel deconvolution method can be implemented to recognize, categorize the main propagating paths and then rectify their time of arrivals. Compared with the phase conjugation-based channel deconvolution method, the proposed approach’s results have fewer sidelobes and higher signal-to-background ratio in the simulation.

Highlights

  • Active acoustic imaging is the technique to locate an object’s scattering strength distribution and characterize it

  • SPARSE RECONSTRUCTION BASED IMAGING METHOD By reviewing Fig.4 and Fig.7(b), it can be found that: (1) The output of matched filter (MF) has a wide main lobe, which may not well separate the reflection and creeping wave; (2) TD-BP using the output of MF produces lots of unwanted ripples and sidelobes

  • This paper focuses on the inverse scattering imaging problems in a bistatic active sonar imaging

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Summary

INTRODUCTION

Active acoustic imaging is the technique to locate an object’s scattering strength distribution and characterize it. J. Jiang et al.: Sparse Reconstruction-Based Inverse Scattering Imaging the linear sampling method (LSM) [18] is applied in the underwater object imaging task with the partial frequency variation approach [19]. This sparse reconstruction-based channel deconvolution imaging is proposed to solve that problem. By reviewing Fig., it can be found that (4) uses the linearized approximation of ||rt − rs|| ≈ Rs + ninc · rt, and ||r − rt|| ≈ Rr − nsct · rt This indicates (4) is originated from the time domain delay-andsum expression:. This paper uses BP’s time-domain equivalence (5) to output the inverse scattering imaging results

SOUND SCATTERING AND INVERSE SCATTERING IMAGING IN A 2D FREE FIELD
SIMULATION IN 2D FREE FIELD SPACE
PHASE CONJUGATION-BASED CHANNEL DECONVOLUTION IMAGING METHOD
CONCLUSION
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