iterative deconvolution
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2021 ◽  
Author(s):  
Viswanath P. Sudarshan ◽  
Pavan Kumar Reddy ◽  
Jayavardhana Gubbi ◽  
Balamuralidhar Purushothaman

Vacuum ◽  
2021 ◽  
Vol 186 ◽  
pp. 110054
Author(s):  
Berthold Jenninger ◽  
Antoine Benoit ◽  
Paolo Chiggiato

Author(s):  
Michael Werth ◽  
Trent Kyono ◽  
Jacob Lucas ◽  
Ian McQuaid ◽  
Justin Fletcher

Author(s):  
Xi Cao ◽  
Bing Chu ◽  
Yu-Xi Liu ◽  
Zhihui Peng ◽  
Re-Bing Wu

Vacuum ◽  
2021 ◽  
Vol 183 ◽  
pp. 109876
Author(s):  
Berthold Jenninger ◽  
Antoine Benoit ◽  
Paolo Chiggiato

MethodsX ◽  
2021 ◽  
Vol 8 ◽  
pp. 101240
Author(s):  
Yu Dong ◽  
H. Christiaan Stronks ◽  
Jeroen J. Briaire ◽  
Johan H.M. Frijns

2020 ◽  
Vol 395 ◽  
pp. 108037 ◽  
Author(s):  
Yu Dong ◽  
Jeroen J. Briaire ◽  
Jan Dirk Biesheuvel ◽  
H. Christiaan Stronks ◽  
Johan H.M. Frijns

Sensors ◽  
2020 ◽  
Vol 20 (10) ◽  
pp. 2844 ◽  
Author(s):  
Chun-Xiao Li ◽  
Ming-Fei Guo ◽  
Hang-Fang Zhao

Matched filtering is widely used in active sonar because of its simplicity and ease of implementation. However, the resolution performance generally depends on the transmitted waveform. Moreover, its detection performance is limited by the high-level sidelobes and seriously degraded in a shallow water environment due to time spread induced by multipath propagation. This paper proposed a method named iterative deconvolution-time reversal (ID-TR), on which the energy of the cross-ambiguity function is modeled, as a convolution of the energy of the auto-ambiguity function of the transmitted signal with the generalized target reflectivity density. Similarly, the generalized target reflectivity density is a convolution of the spread function of channel with the reflectivity density of target as well. The ambiguity caused by the transmitted signal and the spread function of channel are removed by Richardson-Lucy iterative deconvolution and the time reversal processing, respectively. Moreover, this is a special case of the Richardson-Lucy algorithm that the blur function is one-dimensional and time-invariant. Therefore, the iteration deconvolution is actually implemented by the iterative temporal time reversal processing. Due to the iterative time reversal method can focus more and more energy on the strongest target with the iterative number increasing and then the peak-signal power increases, the simulated result shows that the noise reduction can achieve 250 dB in the “ideal” free field environment and 100 dB in a strong multipaths waveguide environment if a 1-ms linear frequency modulation with a 4-kHz frequency bandwidth is transmitted and the number of iteration is 10. Moreover, the range resolution is approximately a delta function. The results of the experiment in a tank show that the noise level is suppressed by more than 70 dB and the reverberation level is suppressed by 3 dB in the case of a single target and the iteration number being 8.


2020 ◽  
Vol 135 (2) ◽  
Author(s):  
Rui Shi ◽  
Xianguo Tuo ◽  
Yi Cheng ◽  
Jianbo Yang ◽  
Mingzhe Liu ◽  
...  

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