CN110488289B - Photoelectric cooperative synthetic aperture radar imaging processing method based on overlapped sub-apertures - Google Patents

Photoelectric cooperative synthetic aperture radar imaging processing method based on overlapped sub-apertures Download PDF

Info

Publication number
CN110488289B
CN110488289B CN201910773690.7A CN201910773690A CN110488289B CN 110488289 B CN110488289 B CN 110488289B CN 201910773690 A CN201910773690 A CN 201910773690A CN 110488289 B CN110488289 B CN 110488289B
Authority
CN
China
Prior art keywords
sub
aperture
sar
apertures
resolution
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Active
Application number
CN201910773690.7A
Other languages
Chinese (zh)
Other versions
CN110488289A (en
Inventor
刘兴钊
袁瑛
高叶盛
袁斌
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Suzhou Xingzhao Defense Research Institute Co ltd
Original Assignee
Suzhou Xingzhao Defense Research Institute Co ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Suzhou Xingzhao Defense Research Institute Co ltd filed Critical Suzhou Xingzhao Defense Research Institute Co ltd
Priority to CN201910773690.7A priority Critical patent/CN110488289B/en
Publication of CN110488289A publication Critical patent/CN110488289A/en
Application granted granted Critical
Publication of CN110488289B publication Critical patent/CN110488289B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S13/00Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
    • G01S13/88Radar or analogous systems specially adapted for specific applications
    • G01S13/89Radar or analogous systems specially adapted for specific applications for mapping or imaging
    • G01S13/90Radar or analogous systems specially adapted for specific applications for mapping or imaging using synthetic aperture techniques, e.g. synthetic aperture radar [SAR] techniques
    • G01S13/9004SAR image acquisition techniques
    • G01S13/9005SAR image acquisition techniques with optical processing of the SAR signals
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S13/00Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
    • G01S13/88Radar or analogous systems specially adapted for specific applications
    • G01S13/89Radar or analogous systems specially adapted for specific applications for mapping or imaging
    • G01S13/90Radar or analogous systems specially adapted for specific applications for mapping or imaging using synthetic aperture techniques, e.g. synthetic aperture radar [SAR] techniques
    • G01S13/9004SAR image acquisition techniques
    • G01S13/9011SAR image acquisition techniques with frequency domain processing of the SAR signals in azimuth

Landscapes

  • Engineering & Computer Science (AREA)
  • Remote Sensing (AREA)
  • Radar, Positioning & Navigation (AREA)
  • Physics & Mathematics (AREA)
  • Signal Processing (AREA)
  • Electromagnetism (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • General Physics & Mathematics (AREA)
  • Radar Systems Or Details Thereof (AREA)

Abstract

The invention relates to a photoelectric cooperative synthetic aperture radar imaging processing method based on overlapping sub-apertures, which comprises the following steps: 1) and (3) aperture segmentation: carrying out aperture segmentation on SAR echo data in a synthetic aperture along the azimuth direction, dividing the SAR echo data into a plurality of sub-aperture data blocks, and carrying out phase shift preprocessing; 2) SAR data imaging processing: respectively and simultaneously modulating the sub-aperture data blocks onto laser beams by adopting a plurality of spatial light modulators in the optical imaging module, and parallelly processing each sub-aperture data block on an optical domain, wherein each path of laser beam parallelly passes through the corresponding optical imaging module, so that the plurality of sub-aperture data blocks loaded on the laser beams simultaneously complete imaging processing, and a plurality of low-resolution SAR images are obtained; 3) and (3) pore diameter synthesis: and synthesizing the plurality of low-resolution SAR images into a final high-resolution SAR image on an optical domain. Compared with the prior art, the invention has the advantages of high resolution, real-time imaging, parallel optical processing and the like.

Description

Photoelectric cooperative synthetic aperture radar imaging processing method based on overlapped sub-apertures
Technical Field
The invention relates to the field of real-time imaging of synthetic aperture radar signals, in particular to a photoelectric cooperative synthetic aperture radar imaging processing method based on overlapped sub-apertures.
Background
Synthetic Aperture Radar (SAR) is a microwave imaging radar that has wide applications in both military and civilian applications. The SAR is used as an important sensor for transmitting information and intelligence, and the timeliness of imaging processing often becomes the key for decision making. In the face of the urgent need of real-time processing, optical processing technology is introduced into the field of SAR signal processing and becomes a research hotspot. The optical processing technology has high-speed parallel processing capability, and complex operation in some SAR signal processing can be realized only by some simple optical elements, so that the technology has the potential of providing real-time imaging processing for the SAR system.
In recent years, many methods have been proposed to implement optical imaging processing of SAR signals, such as the real-time on-board SAR imaging processing system proposed by the canadian national optical research institute. Most of the current methods are only suitable for real-time imaging of low-resolution SAR signals. For the case of high resolution, most methods cannot really realize real-time processing because the processing of the SAR data in one synthetic aperture cannot be completed at a time. These methods only process data that is loaded onto the laser beam by one spatial light modulator at a time. Due to the limitation of the resolution of the spatial light modulator at the present stage, it is impossible to simultaneously and completely load the SAR data in one synthetic aperture onto the laser beam for processing. In order to solve the defects of the existing method and meet the technical requirement of real-time processing, a new SAR signal optical imaging method needs to be developed urgently.
Disclosure of Invention
The invention aims to overcome the defects of the prior art and provide a photoelectric cooperative synthetic aperture radar imaging processing method based on overlapping sub-apertures.
The purpose of the invention can be realized by the following technical scheme:
a photoelectric cooperative synthetic aperture radar imaging processing method based on overlapped sub-apertures comprises the following steps:
1) and (3) aperture segmentation: carrying out aperture segmentation on SAR echo data in a synthetic aperture along the azimuth direction, dividing the SAR echo data into a plurality of sub-aperture data blocks, and carrying out phase shift preprocessing;
2) SAR data imaging processing: respectively and simultaneously modulating the sub-aperture data blocks onto laser beams by adopting a plurality of spatial light modulators in the optical imaging module, and parallelly processing each sub-aperture data block on an optical domain, wherein each path of laser beam parallelly passes through the corresponding optical imaging module, so that the plurality of sub-aperture data blocks loaded on the laser beams simultaneously complete imaging processing, and a plurality of low-resolution SAR images are obtained;
3) and (3) pore diameter synthesis: and synthesizing the plurality of low-resolution SAR images into a final high-resolution SAR image on an optical domain.
In the step 1), the relation between the number of sampling points and the number of sub-apertures of each synthetic aperture is as follows:
N=(S-1)Δ+M
wherein, N is the number of azimuth sampling points in a synthetic aperture, S is the number of sub-apertures, namely the number of sub-aperture data blocks, M is the number of azimuth sampling points of each sub-aperture, and Delta is the number of sampling points at the interval of two adjacent sub-aperture azimuth initial positions.
In the step 1), the data between two adjacent sub-aperture data blocks has an overlapping rate of more than 50% to ensure smooth reorganization of the sub-apertures.
The number of azimuth sampling points of each sub-aperture is smaller than the resolution of the spatial light modulator.
In step 2), in each optical imaging module, a sub-aperture data block is subjected to fourier transform operation, matched filter operation and inverse fourier transform operation, respectively, to form a low-resolution SAR image, specifically:
and performing two-dimensional Fourier transform on the sub-aperture data block, multiplying the sub-aperture data block by a two-dimensional matched filter on a two-dimensional frequency domain, completing the distance direction compression and the azimuth direction compression of the SAR signal at the same time, and focusing to form a low-resolution SAR image after two-dimensional Fourier inverse transformation.
The expression of the sub-aperture data block is as follows:
Figure BDA0002174398350000021
Figure BDA0002174398350000022
where τ and t are range time and azimuth time, ωrAnd ωaIs the distance envelope and the azimuth envelope, A is a constant, c is the speed of light, tcIs the azimuth time when the radar is facing the target, λ is the wavelength, krIs the range chirp rate, R (t) is the instantaneous range of the radar to the target, vsSpeed of radar platform, RcThe slant range of the radar when the radar is closest to the target.
The expression of the two-dimensional matched filter is as follows:
Figure BDA0002174398350000031
wherein f isτAnd ftRespectively, range-wise and azimuth-wise frequencies, f, over a two-dimensional frequency domain0Is the carrier frequency.
The step 3) is specifically as follows:
and respectively executing interpolation and phase shift operation on the low-resolution SAR images of the plurality of sub-apertures, wherein the phase shift operation is used for shifting the frequency spectrums of the low-resolution SAR images of the sub-apertures after interpolation so as to achieve the purpose of frequency spectrum splicing. And outputting the low-resolution SAR images of all the sub-apertures after interpolation and phase shift operation respectively, and finally adding the output results of all the sub-apertures to obtain a high-resolution SAR image.
Compared with the prior art, the invention has the following advantages:
the invention adopts the optical processing technology to realize the imaging processing of SAR data, and has the unique advantage of real-time processing due to the high-speed processing capability of the optical processing technology, and simultaneously, the overlapping subaperture data structure is introduced to enlarge the data processing scale, so that the method is suitable for the processing of massive SAR data, and the method can also process the massive SAR data at high speed and in parallel, therefore, the method still has the capability of real-time imaging processing for high-resolution SAR signals.
Drawings
FIG. 1 is a schematic overall flow chart of the present invention.
Fig. 2 is a schematic diagram of the principle of overlapping subaperture segmentation.
Detailed Description
The invention is described in detail below with reference to the figures and the specific embodiments.
Examples
The present invention will be described in detail with reference to specific examples. The following examples will assist those skilled in the art in further understanding the invention, but are not intended to limit the invention in any way. It should be noted that variations and modifications can be made by persons skilled in the art without departing from the concept of the invention. All falling within the scope of the present invention.
In order to achieve the purpose, the technical scheme adopted by the invention is as follows:
the overall flow diagram of the technical scheme is shown in figure 1. And carrying out aperture segmentation on SAR echo data in one synthetic aperture along the azimuth direction, and dividing the SAR echo data into a plurality of sub-aperture data blocks. The data between two adjacent sub-aperture data blocks have a certain overlapping rate. Then, the sub-aperture data blocks are modulated onto the laser beam separately and simultaneously by using a plurality of spatial light modulators. The sub-aperture data blocks are then processed in parallel in the optical domain. And as each path of laser beam passes through the plurality of optical imaging modules in parallel, the sub-aperture data blocks loaded on the laser beam complete imaging processing at the same time to obtain a plurality of low-resolution SAR images. And finally, synthesizing the plurality of low-resolution SAR images into a final high-resolution SAR image on an optical domain. This step can be achieved by passing the laser beam through a series of optical elements. The final SAR image may be acquired and digitized by a camera.
The technical scheme can be divided into three steps of aperture segmentation, SAR data imaging processing and aperture synthesis. The specific implementation steps are as follows:
the method comprises the following steps: and (5) dividing the aperture.
And carrying out aperture segmentation on SAR echo data of a full synthetic aperture along the azimuth direction, and dividing the SAR echo data into a plurality of sub-aperture data blocks. The data between two adjacent sub-aperture data blocks have a certain overlap ratio to ensure smooth reorganization of the sub-apertures. The specific division is shown in fig. 2. N is the number of azimuth sampling points in one synthetic aperture, S is the number of sub-apertures, M is the number of azimuth sampling points of each sub-aperture, and delta is the number of sampling points at the interval of the azimuth initial positions of two adjacent sub-apertures. (M-Delta) is the number of overlapping points between adjacent sub-apertures. The relationship between the number of sampling points and the number of sub-apertures for a synthetic aperture is as follows:
N=(S-1)Δ+M
the number of subaperture segmentations can be determined in accordance with the above equation. Firstly, setting an overlapping rate, wherein the overlapping rate is generally set to be 50% or more, and then setting the number of sampling points of each sub-aperture, wherein the number of the set sampling points does not exceed the resolution of the spatial light modulator. And then, the number S of the sub-apertures can be calculated according to the number of sampling points of one synthetic aperture. After the SAR data is divided into S sub-aperture data blocks, each sub-aperture data needs to be preprocessed. In pre-processing, each sub-aperture data block is phase shifted such that the spectral center of each sub-aperture is shifted to zero frequency. Next, the sub-aperture data blocks are loaded onto the laser beam simultaneously using S spatial light modulators.
Step two: and (5) SAR data imaging processing.
And the S sub-aperture data blocks loaded on the laser beams respectively complete imaging processing along with the S laser beams parallelly passing through the S optical imaging modules. Each sub-aperture data block imaging processing procedure comprises a Fourier transform operation, a matched filtering operation and an inverse Fourier transform operation. The specific flow of the imaging process is to perform two-dimensional fourier transform on the sub-aperture data block. And then multiplying the SAR signal by a two-dimensional matched filter on a two-dimensional frequency domain, and simultaneously completing the distance direction compression and the azimuth direction compression of the SAR signal through the step. Then, through two-dimensional inverse Fourier transform, a SAR image can be focused and formed, but the SAR image is low-resolution. The above operations required in the imaging process can be realized by the optical elements. And after the second step, S low-resolution SAR images can be obtained.
The form of the subaperture data block and its corresponding two-dimensional matched filter is given below.
The expression for the sub-aperture data block is as follows:
Figure BDA0002174398350000051
wherein R (t) is approximately represented by:
Figure BDA0002174398350000052
the expression for the two-dimensional matched filter is as follows:
Figure BDA0002174398350000053
where τ and t represent range-wise time and azimuth-wise time; omegarAnd ωaRepresenting a range-wise envelope and an azimuth-wise envelope; a is a constant; c is the speed of light; t is tcIs the azimuth time when the radar is facing the target; λ is the wavelength; k is a radical ofrIs the distance-to-chirp slope; r (t) is the instantaneous distance of the radar from the target. v. ofsIs the speed of the radar platform; r iscIs the slant distance, f, of the radar closest to the targetτAnd ftRespectively representing distance direction frequency and azimuth direction frequency on a two-dimensional frequency domain; f. of0Representing the carrier frequency.
Step three: and (4) aperture synthesis.
The method comprises the steps of processing the frequency spectrums of each sub-aperture data, and then splicing the frequency spectrums of all the sub-apertures to fit the frequency spectrum of the full synthetic aperture data to obtain the SAR image with high resolution. The specific process is that firstly, the interpolation and phase shift operation are respectively executed on the low-resolution SAR images of S sub-apertures obtained in the step two, wherein the phase shift operation is used for shifting the frequency spectrum of the low-resolution SAR images of each sub-aperture after interpolation so as to achieve the purpose of frequency spectrum splicing. And outputting the low-resolution SAR images of all the sub-apertures after interpolation and phase shift operation respectively. And then, adding the output results of all the sub-apertures to obtain a high-resolution SAR image. The operations required in the step can be realized by optical elements, and the obtained SAR image can be collected and digitalized by a camera. After the third step, a high-resolution SAR image can be obtained.
Description of spatial light modulators
Spatial light modulator, its english name is spatial light modulator, SLM. It is a device that modulates the spatial distribution of light waves. The device is usually composed of many small individual cells distributed in a two-dimensional matrix. The individual cells are also called pixels. Each pixel is capable of independently modulating the light beam illuminated thereon such that a certain characteristic of the light wave varies according to the law of the modulation signal. Modulating the amplitude and phase characteristics of the beam can be accomplished by modulating a complex signal (e.g., a SAR signal) onto the laser beam. A common spatial light modulator has a resolution of 4096 × 2048 pixels and 1920 × 1080 pixels.
The foregoing description of specific embodiments of the present invention has been presented. It is to be understood that the present invention is not limited to the specific embodiments described above, and that various changes or modifications may be made by one skilled in the art within the scope of the appended claims without departing from the spirit of the invention. The embodiments and features of the embodiments of the present application may be combined with each other arbitrarily without conflict.

Claims (1)

1. A photoelectric cooperative synthetic aperture radar imaging processing method based on overlapped sub-apertures is characterized by comprising the following steps:
1) and (3) aperture segmentation: carrying out aperture segmentation on SAR echo data in a synthetic aperture along the azimuth direction, dividing the SAR echo data into a plurality of sub-aperture data blocks, and then carrying out phase shift preprocessing, wherein the relational expression between the number of sampling points and the number of sub-apertures of each synthetic aperture is as follows:
N=(S-1)Δ+M
n is the number of azimuth sampling points in a synthetic aperture, S is the number of sub-apertures, namely the number of sub-aperture data blocks, M is the number of azimuth sampling points of each sub-aperture, Delta is the number of sampling points spaced at the azimuth starting positions of two adjacent sub-apertures, the number of azimuth sampling points of each sub-aperture is smaller than the resolution of the spatial light modulator, and the data between the two adjacent sub-aperture data blocks has an overlapping rate of more than 50% so as to ensure the smooth recombination of the sub-apertures;
2) SAR data imaging processing: adopt a plurality of spatial light modulators in the optical imaging module to modulate the subaperture data block respectively and simultaneously on the laser beam, and parallel processing each subaperture data block on the optical domain, each path of laser beam passes through the corresponding optical imaging module in parallel, make a plurality of subaperture data blocks loaded on the laser beam accomplish the imaging processing simultaneously, obtain a plurality of SAR images of low resolution, in each optical imaging module, form a SAR image of low resolution after carrying out Fourier transform operation, matched filter operation and Fourier inverse transform operation respectively to the subaperture data block, specifically do:
performing two-dimensional Fourier transform on the sub-aperture data block, multiplying the sub-aperture data block by a two-dimensional matched filter on a two-dimensional frequency domain, completing the distance direction compression and the azimuth direction compression of the SAR signal at the same time, and focusing to form a low-resolution SAR image after the two-dimensional Fourier transform;
the expression of the sub-aperture data block is as follows:
Figure FDA0003302915450000011
Figure FDA0003302915450000012
where τ and t are range time and azimuth time, ωrAnd omegaaIs a distance envelope and an azimuth envelope, A is a constant, c is the speed of light, tcIs the azimuth time when the radar is facing the target, λ is the wavelength, krFor range-to-chirp slope, R (t) is the instantaneous range of the radar to the target, vsSpeed of radar platform, RcThe slant distance when the radar is closest to the target;
the expression of the two-dimensional matched filter is as follows:
Figure FDA0003302915450000021
wherein f isτAnd ftRespectively, range-wise and azimuth-wise frequencies, f, over a two-dimensional frequency domain0Is the carrier frequency;
3) and (3) pore diameter synthesis: synthesizing a plurality of low-resolution SAR images into a final high-resolution SAR image on an optical domain, specifically:
and respectively executing interpolation and phase shift operation on the low-resolution SAR images of the plurality of sub-apertures, wherein the phase shift operation is used for shifting the frequency spectrum of the low-resolution SAR image of each sub-aperture after interpolation so as to achieve the purpose of frequency spectrum splicing, outputting the low-resolution SAR images of all sub-apertures after interpolation and phase shift operation, and finally adding the output results of all sub-apertures to obtain a high-resolution SAR image.
CN201910773690.7A 2019-08-21 2019-08-21 Photoelectric cooperative synthetic aperture radar imaging processing method based on overlapped sub-apertures Active CN110488289B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201910773690.7A CN110488289B (en) 2019-08-21 2019-08-21 Photoelectric cooperative synthetic aperture radar imaging processing method based on overlapped sub-apertures

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201910773690.7A CN110488289B (en) 2019-08-21 2019-08-21 Photoelectric cooperative synthetic aperture radar imaging processing method based on overlapped sub-apertures

Publications (2)

Publication Number Publication Date
CN110488289A CN110488289A (en) 2019-11-22
CN110488289B true CN110488289B (en) 2022-07-15

Family

ID=68551788

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201910773690.7A Active CN110488289B (en) 2019-08-21 2019-08-21 Photoelectric cooperative synthetic aperture radar imaging processing method based on overlapped sub-apertures

Country Status (1)

Country Link
CN (1) CN110488289B (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111538005B (en) * 2020-05-13 2023-03-24 西安电子科技大学 SAR front-side-looking imaging method based on FPGA and multiple multi-core DSPs
CN114839633B (en) * 2022-07-01 2022-09-20 南京隼眼电子科技有限公司 Millimeter wave synthetic aperture radar imaging method and device and storage medium
CN117745779B (en) * 2024-02-19 2024-05-07 中国科学院空天信息创新研究院 Optical and SAR common aperture consistency imaging method

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1997043664A1 (en) * 1996-05-10 1997-11-20 Environmental Research Institute Of Michigan Subchirp processing method
CN104391297A (en) * 2014-11-17 2015-03-04 南京航空航天大学 Sub-aperture partition PFA (Polar Format Algorithm) radar imaging method
CN109633638A (en) * 2018-11-19 2019-04-16 上海无线电设备研究所 A kind of wide-angle SAR super-resolution imaging method based on EM scatter model

Family Cites Families (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5122803A (en) * 1991-11-06 1992-06-16 The United States Of America As Represented By The Secretary Of The Army Moving target imaging synthetic aperture radar
SE512532C2 (en) * 1999-02-26 2000-03-27 Foersvarets Forskningsanstalt Use a SAR radar to detect objects that change over time
US8274422B1 (en) * 2010-07-13 2012-09-25 The Boeing Company Interactive synthetic aperture radar processor and system and method for generating images
CN101984363B (en) * 2010-10-27 2013-03-06 南京航空航天大学 Ultrahigh-resolution synthetic aperture radar (SAR) imaging method based on frequency-stepped system
CN102288964B (en) * 2011-08-19 2013-03-20 中国资源卫星应用中心 Imaging processing method for spaceborne high-resolution synthetic aperture radar
CN103728618B (en) * 2014-01-16 2015-12-30 中国科学院电子学研究所 The satellite-borne SAR system implementation method of a kind of high resolving power, wide swath
CN105137432B (en) * 2015-08-19 2018-07-03 上海交通大学 Ground synthetic aperture radar three-dimensional imaging method based on orthogonal image registration
CN108226925A (en) * 2017-12-01 2018-06-29 清华大学 A kind of overlapped sub-aperture algorithm suitable for missile-borne strabismus time-varying parameter SAR before big
CN108205135B (en) * 2018-01-22 2022-03-04 西安电子科技大学 Radar video imaging method based on non-interpolation fusion fast backward projection

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1997043664A1 (en) * 1996-05-10 1997-11-20 Environmental Research Institute Of Michigan Subchirp processing method
CN104391297A (en) * 2014-11-17 2015-03-04 南京航空航天大学 Sub-aperture partition PFA (Polar Format Algorithm) radar imaging method
CN109633638A (en) * 2018-11-19 2019-04-16 上海无线电设备研究所 A kind of wide-angle SAR super-resolution imaging method based on EM scatter model

Non-Patent Citations (5)

* Cited by examiner, † Cited by third party
Title
A optronic SAR processor with high-speed and high-precision phase modulation;Lei Liu,Yesheng Gao,Kaizhi Wang,Xingzhao Liu;《 2016 IEEE International Geoscience and Remote Sensing Symposium (IGARSS)》;IEEE;20161103;第1126-1129页 *
Azimuth Overlapped Subaperture Algorithm in Frequency Domain for Highly Squinted Synthetic Aperture Radar;TANG Yu,ZHANG Bo,XING Meng-dao;《 IEEE Geoscience and Remote Sensing Letters》;20121026;第10卷(第4期);第692-696页 *
Lei Liu, Yesheng Gao, Xingzhao Liu.OPTRONIC HIGH-RESOLUTION SAR PROCESSING WITH THE CAPABILITY OF FULL-RESOLUTION IMAGING.《IGARSS 2018 - 2018 IEEE International Geoscience and Remote Sensing Symposium》.2018,第8913-8916页. *
OPTRONIC HIGH-RESOLUTION SAR PROCESSING WITH THE CAPABILITY OF FULL-RESOLUTION IMAGING;Lei Liu, Yesheng Gao, Xingzhao Liu;《IGARSS 2018 - 2018 IEEE International Geoscience and Remote Sensing Symposium》;20181105;第8913-8916页 *
基于光电协同的雷达实时信号处理技术;刘兴钊,高叶盛;《数据采集与处理》;20170715;第658-666页 *

Also Published As

Publication number Publication date
CN110488289A (en) 2019-11-22

Similar Documents

Publication Publication Date Title
CN110488289B (en) Photoelectric cooperative synthetic aperture radar imaging processing method based on overlapped sub-apertures
US9134414B2 (en) Method and apparatus for determining a doppler centroid in a synthetic aperture imaging system
CN111175750A (en) Imaging method, device, equipment and storage medium of synthetic aperture radar
EP0544533B1 (en) Improved ISAR imaging radar system
CN101980049B (en) Fresnel telescope imaging laser radar
US10690767B2 (en) System and method for synthetic aperture radar image formation
US3519331A (en) Two-dimensional optical data processor
CN107102328B (en) FPGA-based real-time imaging signal processing method and FPGA
Gromek et al. Passive SAR imaging using DVB‐T illumination for airborne applications
CN114529830A (en) Remote sensing image space-time fusion method based on mixed convolution network
CN110488290A (en) The photoelectric-synergetic processing system of high resolution synthetic aperture radar signal panoramic imagery
CN111751799A (en) Ultra-wideband multi-target detection method
Martin et al. Design and performance of a distributed aperture millimeter-wave imaging system using optical upconversion
Wang et al. Study on processing synthetic aperture radar data based on an optical 4f system for fast imaging
Xin et al. A wide-field SAR polar format algorithm based on quadtree sub-image segmentation
Ausherman Digital versus optical techniques in synthetic aperture radar (SAR) data processing
CN115755046A (en) Extended PFA algorithm for imaging large azimuth width of stripe SAR
CN113189547B (en) SAR imaging method and system based on synthetic bandwidth frequency scaling
US5566382A (en) Mutiple-clock controlled spatial light modulator
CN111220974B (en) Low-complexity frequency domain splicing method based on frequency modulation stepping pulse signals
Leith A short history of the Optics Group of the Willow Run Laboratories
Liu et al. Optronic high-resolution sar processing with the capability of full-resolution imaging
Yang et al. Compact optical real-time imaging system for high-resolution SAR data based on autofocusing
Lebreton et al. Holographic processing of wideband antenna data
US11515946B1 (en) System and method for analog estimation and streaming of a spectral correlation function (SCF)

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant