Radar moving target radon-fractional Fourier transform long-time phase-coherent accumulation detection method
A fractional Fourier, coherent accumulation technology, applied in radio wave measurement systems, instruments, etc., can solve the problems of uncomfortable signal processing, signal accumulation efficiency and low signal noise, affecting the accumulation effect, etc., to improve the output signal noise ( noise) ratio, suppressing background clutter and noise, and improving estimation accuracy
Patent Information
- Authority / Receiving Office
- CN · China
- Current Assignee / Owner
- Publication Date
- 2013-06-26
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Abstract
Description
1. Technical field
[0001] The invention belongs to the technical field of radar signal processing and detection. More specifically, the invention relates to a radar moving target Radon-fractional Fourier transform long-term coherent accumulation detection method, which can be used for radar detection of weak moving targets in complex environments deal with. 2. Background technology
[0002] With the development of science and technology, especially the continuous development of high-speed targets and the increasing maturity of stealth technology, robust and effective radar moving target detection has always been a difficult problem in the field of radar signal processing. Research on signal processing to improve the ability of radar to detect weak moving targets method is important. The complexity of target detection not only comes from the target itself, but also is affected by the increasingly complex electromagnetic environment and clutter background. There are many type...
Examples
Embodiment Construction
[0027] In order to explain the range migration and Doppler migration effects involved in the present invention, the following derivation is first made.
[0028] In order to obtain high resolution and reduce the effective bandwidth, it is assumed that the coherent system radar transmits a linear frequency modulation (Linear Frequency Modulation, LFM) signal
[0029] s t ( t ) = rect ( t T p ) exp { j 2 π [ f c t + 1 2 kt 2 ] }
[0030] In the formula, rect ( u ) = ...