TY - GEN
T1 - High-resolution sonar imaging using sparse transmitting and dense receiving arrays
AU - Liu, Xionghou
AU - Sun, Chao
AU - Xiang, Longfeng
AU - Yang, Yixin
AU - Kong, Dezhi
AU - Yao, Yuan
N1 - Publisher Copyright:
© 2018 IEEE.
PY - 2018/12/4
Y1 - 2018/12/4
N2 - An imaging sonar usually uses a large aperture hydrophone array to obtain a fine angle resolution, leading to a high system cost. To obtain a high angle resolution with a limited number of elements, we propose a new imaging method which uses a sparse M-element transmitting uniform linear array (ULA) and a dense N-element receiving ULA. The inter-element spacing of the transmitting ULA (i.e., dt) and that of the receiving ULA (i.e., dr) satisfy dt=Ndr. The sparse transmitting ULA produces multiple grating lobes to discretely illuminate the target scene, and the receiving beams (produced by the dense ULA) are steered to these grating lobes. Thus, in a ping the scanning beam number is equal to that of grating lobes. Meanwhile, the multi-ping illumination is utilized to produce enough grating lobes (by changing the transmitting mainlobe direction for different pings) to cover the target scene. Moreover, the array manifold errors of the transmitting and receiving ULAs are also taken into consideration, and the relative influences on the beampattern and the imaging result are analyzed. Numerical simulation show that the proposed method has a similar imaging ability to the MNelement ULA by using only (M+N) physical elements.
AB - An imaging sonar usually uses a large aperture hydrophone array to obtain a fine angle resolution, leading to a high system cost. To obtain a high angle resolution with a limited number of elements, we propose a new imaging method which uses a sparse M-element transmitting uniform linear array (ULA) and a dense N-element receiving ULA. The inter-element spacing of the transmitting ULA (i.e., dt) and that of the receiving ULA (i.e., dr) satisfy dt=Ndr. The sparse transmitting ULA produces multiple grating lobes to discretely illuminate the target scene, and the receiving beams (produced by the dense ULA) are steered to these grating lobes. Thus, in a ping the scanning beam number is equal to that of grating lobes. Meanwhile, the multi-ping illumination is utilized to produce enough grating lobes (by changing the transmitting mainlobe direction for different pings) to cover the target scene. Moreover, the array manifold errors of the transmitting and receiving ULAs are also taken into consideration, and the relative influences on the beampattern and the imaging result are analyzed. Numerical simulation show that the proposed method has a similar imaging ability to the MNelement ULA by using only (M+N) physical elements.
KW - Array signal processing
KW - Sonar imaging
KW - Sparse array
KW - Underwater acoustics
UR - http://www.scopus.com/inward/record.url?scp=85060278893&partnerID=8YFLogxK
U2 - 10.1109/OCEANSKOBE.2018.8559169
DO - 10.1109/OCEANSKOBE.2018.8559169
M3 - 会议稿件
AN - SCOPUS:85060278893
T3 - 2018 OCEANS - MTS/IEEE Kobe Techno-Oceans, OCEANS - Kobe 2018
BT - 2018 OCEANS - MTS/IEEE Kobe Techno-Oceans, OCEANS - Kobe 2018
PB - Institute of Electrical and Electronics Engineers Inc.
T2 - 2018 OCEANS - MTS/IEEE Kobe Techno-Oceans, OCEANS - Kobe 2018
Y2 - 28 May 2018 through 31 May 2018
ER -