CN107728130A - Multi-channel wide Amplitude Composition aperture laser imaging radar receive-transmit system - Google Patents

Multi-channel wide Amplitude Composition aperture laser imaging radar receive-transmit system Download PDF

Info

Publication number
CN107728130A
CN107728130A CN201710828948.XA CN201710828948A CN107728130A CN 107728130 A CN107728130 A CN 107728130A CN 201710828948 A CN201710828948 A CN 201710828948A CN 107728130 A CN107728130 A CN 107728130A
Authority
CN
China
Prior art keywords
fiber
input
output end
array
fiber amplifier
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.)
Granted
Application number
CN201710828948.XA
Other languages
Chinese (zh)
Other versions
CN107728130B (en
Inventor
周煜
张波
孙建锋
李光远
张国
许蒙蒙
劳陈哲
贺红雨
毛奥
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 Xuanguang Semiconductor Technology Co ltd
Original Assignee
Shanghai Institute of Optics and Fine Mechanics of CAS
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 Shanghai Institute of Optics and Fine Mechanics of CAS filed Critical Shanghai Institute of Optics and Fine Mechanics of CAS
Priority to CN201710828948.XA priority Critical patent/CN107728130B/en
Publication of CN107728130A publication Critical patent/CN107728130A/en
Application granted granted Critical
Publication of CN107728130B publication Critical patent/CN107728130B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

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
    • G01S7/00Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/48Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S17/00
    • G01S7/481Constructional features, e.g. arrangements of optical elements
    • G01S7/4811Constructional features, e.g. arrangements of optical elements common to transmitter and receiver

Landscapes

  • Engineering & Computer Science (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Radar, Positioning & Navigation (AREA)
  • Remote Sensing (AREA)
  • Optical Radar Systems And Details Thereof (AREA)

Abstract

A kind of multi-channel wide Amplitude Composition aperture laser imaging radar receive-transmit system, emission system, which is formed, includes LASER Light Source, frequency modulator, AWG, fiber optic splitter, fiber amplifier group, fiber array device, lens, the first beam splitter, Brewster prism shrink beam device, and reception system, which is formed, includes the second beam splitter, receiving lens, detector array, capture card and computer.The present invention increases the optics toes and imaging bar amplitude of target face by way of multiple-input and multiple-output, and this will have very important significance to remote high-resolution airbome synthetic aperture laser imaging radar.

Description

Multi-channel wide Amplitude Composition aperture laser imaging radar receive-transmit system
Technical field
The present invention relates to synthetic aperture laser imaging radar, particularly a kind of multi-channel wide Amplitude Composition aperture laser imaging Radar transmit-receive system, have to the airbome synthetic aperture laser imaging radar of the wide bar amplitude of remote high-resolution very important Meaning.
Background technology
Synthetic aperture laser imaging radar (Synthetic Aperture Imaging Ladar, abbreviation SAIL) is can Unique optical imagery Observations Means of Centimeter Level imaging resolution are being obtained at a distance, and its principle takes from the conjunction of RF application Into aperture laser radar (Synthetic Aperture Radar, abbreviation SAR) principle, by contrast, optical wavelength is relatively micro- The small 3-6 number magnitude of ripple wavelength, this results in SAIL resolution ratio SAR to want the high 3-6 order of magnitude, meanwhile, direct band The problem of coming is that visual field wants the small 2-5 order of magnitude.The current airborne SAIL realized both at home and abroad maximum imaging viewing field is 4.8mrad, much smaller than the visual field of SAR and CCD camera (Lu Zhiyong, Zhou Yu, Sun Jianfeng, Luan Zhu, Wang Lijuan, Xu Qian, Li Guangyuan, The airborne Orthoptic synthetic aperture laser imaging radar outfields of Zhang Guo, Liu Li people and flight experiment [J] Chinese lasers, 2017,44 (01):265-271.)。
Prior art (Yu Tang, Bao Qin, Yun Yan, and Mengdao Xing, " Multiple-input multiple-output synthetic aperture ladar system for wide-swath with high Azimuth resolution, " Appl.Opt.55,1401-1405 (2016)) propose a kind of orientation MIMO SAL bodies System, synthesized using the multi-channel data of orientation, solve the contradiction of orientation high-resolution and distance to mapping bandwidth.But It is that the program does not provide the R-T unit of the Synthetic Aperture Laser Radar of MIMO, and does not account for launching in light path The influence that dutycycle between the covering and fibre core of launching fiber is imaged to far field.
Multiple light beams are simultaneously emitted by the SAIL emitters of MIMO, the transmitting light as the SAIL of MIMO Road, transmitting light pass through optical fiber output.If the SAIL of MIMO launching fiber with straight rail to carrying out on vertical direction During arrangement, due to the presence of fibre cladding, target face is not arrived by full illumination upwards in cross rail, as SAIL in straight rail to entering During row Scan, into picture be object each discrete local picture.
In view of problem above, we have carried out grinding for multi-channel wide Amplitude Composition aperture laser imaging radar receive-transmit system Study carefully.This will have very important significance to the airbome synthetic aperture laser imaging radar of the wide bar amplitude of remote high-resolution.
The content of the invention
Present invention aims at further development synthetic aperture laser imaging radar, a kind of multi-channel wide Amplitude Composition is proposed Aperture laser imaging radar receive-transmit system.The system features are that it increases target face by way of multiple-input and multiple-output Optics toes and imaging bar amplitude, and the dutycycle in transmitting light path between the covering and fibre core of launching fiber is considered to remote The influence of field imaging, give the inclination arrangement of optical fiber in fiber array device.In addition, for coherent detection system, receive Visual field is restricted by antenna law, and Receiver aperture is inversely proportional with visual field.And in order to improve reception resolution ratio, system power dissipation is reduced, It it is generally desirable to use collection with large aperture.In order to solve the contradiction between Receiver aperture and visual field, present invention uses array heterodyne Reception mode.This will have very important significance to remote high-resolution airbome synthetic aperture laser imaging radar.
The technical solution of the present invention is as follows:
A kind of multi-channel wide Amplitude Composition aperture laser imaging radar receive-transmit system, including emission system and reception system, Feature is,
Described emission system includes LASER Light Source, frequency modulator, AWG, fiber optic splitter, optical fiber Amplifier group, fiber array device, lens, the first beam splitter, Brewster prism shrink beam device, reception system, which is formed, includes second point Beam device, detector array, capture card and computer;The output end of described LASER Light Source and the first of described frequency modulator Input is connected, and the output end of described AWG is connected with the second input of described frequency modulator, institute The output end for the frequency modulator stated is connected with the input of described fiber optic splitter, and the first of described fiber optic splitter is defeated Go out end, the second output end, the 3rd the n-th output end of output end ... are put with the first optical fiber in described fiber amplifier group respectively The big input of device, the input of the second fiber amplifier, the fiber amplifier of input ... n-th of the 3rd fiber amplifier Input is connected, the output of the output end, the second fiber amplifier of the first fiber amplifier in described fiber amplifier group End, the 3rd fiber amplifier the fiber amplifier of output end ... n-th output end respectively with described fiber array device the One input, the second input, the 3rd the n-th input of input ... are connected, the output end of described fiber array device and institute The input for the lens stated is connected, and the output end of described lens is connected with the input of the first described beam splitter;Described First output end of the first beam splitter is connected with the input of described Brewster prism shrink beam device, described Brewster rib The signal of the output end output of mirror shrink beam device is transmission signal, and described n is more than 3 positive integer;
Described reception system, which is formed, includes receiving lens, the second beam splitter, detector array, capture card and computer; Echo-signal of the transmission signal after target face enters the input of described receiving lens, the output of described receiving lens The first input end in the second described beam splitter is held to be connected, the second output end of the first described beam splitter and described second Second input of beam splitter is connected, the output end of the second described beam splitter and the input phase of described detector array Even, the output end of described detector array is connected with the input of described capture card, the output end of described capture card and The input of described computer is connected.
Described Brewster prism shrink beam device is made up of the first cylinder wedge-shaped mirrors and the second cylinder wedge-shaped mirrors;
The light that the fibre core of optical fiber comes out in described fiber array device cross rail must meet most great achievement upwards at far field Overlapped in the case of slice amplitude to ensure target by full illumination, then need to consider launching fiber in transmitting light path The influence that dutycycle between covering and fibre core is imaged to far field.The diameter of every optical fiber is D in fiber array device, and fibre core is straight Footpath is d, and the numbering of n root optical fiber is respectively:f1,f2,..,fn, the upward distance values dr of the cross rails of two adjacent optical fiber of subscript It is fixed, it is η times of core diameter, wherein 0 < η < 1, the n roots launching fiber in described fiber array device 6 presses following arrangement side Formula is arranged:Keep tangent between adjacent two optical fiber, launching fiber arrangement mode L is L=(f1,f2,..,fn), n root light Angle theta between the line and horizontal line at fine center meets following relation:
The arrangement mode of launching fiber can ensure that launch light cross rail at far field exists upwards in described fiber array device Meet to overlap in the case of maximum imaging bar amplitude, then target can be by complete imaging.
The array element of described detector array is identical with the quantity of the launching fiber of described fiber array device, arrangement mode Unanimously, closely coupled between each array element, the angle theta between the line and horizontal line at the center of n array element meets following relation:
Further, since flashlight after being collimated through described diversing lens by described Brewster prism shrink beam Device realize cross rail near field compression, far field expands.Then the upward near field of corresponding cross rail have compressed how many times, will be opened up on far field Same multiple is opened up, then similarly increases corresponding multiple on described detector array cross rail detection viewing field.If Receiver aperture To launch a times of bore, the compression ratio of described Brewster prism shrink beam device is b, then described detector array test surface The unit array element of single launching fiber is to the array relationship upward with cross rail in straight rail corresponding to upper:a×ab.
Pass through local oscillator light of the first described beam splitter reflection light as receives echo-signal, the local oscillator light in emission system In n beams light correspond to each passage that cross rail is upward in described detector array respectively, local oscillator light from target face with reflecting The echo-signal returned carries out heterodyne reception by described detector array.
Compared with prior art, the beneficial effects of the invention are as follows:
1. the present invention increases the optics toes and imaging bar amplitude of target face by the way of multiple-input and multiple-output, expand Visual field.
2. the dutycycle that the present invention considers in fiber array device between the covering and fibre core of launching fiber is imaged to far field Influence, give the inclination arrangement of optical fiber in fiber array device.The arrangement mode of launching fiber can ensure target into It is the complete imaging of target during picture, rather than discrete local picture.
2. present invention uses array heterodyne reception mode, solve in coherent detection system between Receiver aperture and visual field Contradiction, further expand imaging viewing field.
Brief description of the drawings
Fig. 1 is the structural representation of multi-channel wide Amplitude Composition aperture laser imaging radar receive-transmit system of the present invention.
Fig. 2 is optical fiber in fiber array device in multi-channel wide Amplitude Composition aperture laser imaging radar receive-transmit system of the present invention The structural representation (n=16) of arrangement.
Fig. 3 is that fiber array device launches light in multi-channel wide Amplitude Composition aperture laser imaging radar receive-transmit system of the present invention The light of fibre transmitting is imaged on the upward projection of cross rail in the imaging (n=16) in far field, (a) far field imaging schematic diagram, (b) far field.
Fig. 4 is the battle array in detector array in multi-channel wide Amplitude Composition aperture laser imaging radar receive-transmit system of the present invention First layout viewing (n=4).
Embodiment
The present invention is described in further detail with reference to the accompanying drawings and examples, but the guarantor of the present invention should not be limited with this Protect scope.
Fig. 1 is the structural representation of multi-channel wide Amplitude Composition aperture laser imaging radar receive-transmit system of the present invention.By scheming It can be seen that multi-channel wide Amplitude Composition aperture laser imaging radar receive-transmit system of the present invention, including emission system and reception system,
Described emission system include LASER Light Source 1, frequency modulator 2, AWG 3, fiber optic splitter 4, Fiber amplifier group 5, fiber array device 6, diversing lens 7, the first beam splitter 8 and Brewster prism shrink beam device 9;
The output end of described LASER Light Source 1 is connected with the first input end of described frequency modulator 2, and described is any The output end of waveform generator 3 is connected with the second input of described frequency modulator 2, described frequency modulator 2 it is defeated Go out end with the input of described fiber optic splitter 4 to be connected, the first output end of described fiber optic splitter 4, the second output end, 3rd output end ..., the input with the first fiber amplifier 51 in described fiber amplifier group 5 respectively of the n-th output end End, the input of the second fiber amplifier 52, the 3rd fiber amplifier 53 input ..., the n-th fiber amplifier 5n it is defeated Enter end to be connected, the output end of the first fiber amplifier 51 in described fiber amplifier group 5, the second fiber amplifier 52 Output end, the output end of the 3rd fiber amplifier 53 ..., the n-th fiber amplifier 5n output end respectively with described optical fiber The first input end of array device 6, the second input, the 3rd input ..., the n-th input be connected, described fiber array device Incident light is divided into transmitted light by 6 output light through described lens 7 and the first described beam splitter 8, first beam splitter 8 successively And reflected light, the described output of Brewster prism shrink beam device 9 of described transmitted light warp are transmission signal, described n be 3 with On positive integer;
Described reception system, which is formed, includes receiving lens 10, the second beam splitter 11, detector array 12, capture card 13 With computer 14;
The echo-signal that described transmission signal reflects through target face passes through described receiving lens 10, through described successively Second beam splitter 11 simultaneously enters after described the second beam splitter 11 reflection described with the reflected light of the first described beam splitter 8 Detector array 12, the input phase of the acquired card 13 of output end and described computer 14 of described detector array 12 Even.
The multi-channel wide Amplitude Composition aperture laser imaging radar receive-transmit system is characterised by described Brewster prism Shrink beam device 9 is made up of the first cylinder wedge-shaped mirrors 91 and the second cylinder wedge-shaped mirrors 92;
The light that the fibre core of optical fiber comes out in described fiber array device 6 cross rail must meet most great achievement upwards at far field Overlapped in the case of slice amplitude to ensure target by full illumination, then need to consider launching fiber in transmitting light path The influence that dutycycle between covering and fibre core is imaged to far field.The diameter of every optical fiber of fiber array device 6 is D, fibre core Diameter is d, and the numbering of n root optical fiber is respectively:f1,f2,..,fn, the upward distance values of the cross rails of two adjacent optical fiber of subscript Dr is fixed, and is η times of core diameter, wherein 0 < η < 1, the n roots launching fiber of described fiber array device 6 presses following arrangement side Formula is arranged:Keep tangent between adjacent two optical fiber, launching fiber arrangement mode L is L=(f1,f2,..,fn), n root light Angle theta between the line and horizontal line at fine center meets following relation:
The arrangement mode of launching fiber can ensure that launch light cross rail at far field exists upwards in described fiber array device 6 Meet to overlap in the case of maximum imaging bar amplitude, then target can be by complete imaging.
The array element of described detector array 12 is identical with the quantity of the launching fiber of described fiber array device 6, arrangement Mode is consistent, closely coupled between each array element, and the angle theta between the line and horizontal line at the center of n array element meets as follows Relation:
Further, since flashlight is realized after being collimated through lens by described Brewster prism shrink beam device 9 Cross rail near field compression, far field expands.Then the upward near field of corresponding cross rail have compressed how many times, will be expanded equally on far field Multiple, then similarly increase corresponding multiple on the described cross rail detection viewing field of detector array 12.If Receiver aperture is transmitting A times of bore, the compression ratio of described Brewster prism shrink beam device 9 is b, then right on the described test surface of detector array 12 The unit array element for the single launching fiber answered is to the array relationship upward with cross rail in straight rail:a×ab.
Pass through local oscillator light of the described reflected light of the first beam splitter 8 as receives echo-signal, the local oscillator in emission system N beams light in light corresponds to each array element that cross rail is upward in described detector array 12 respectively, local oscillator light with from target face The echo-signal reflected carries out heterodyne reception, the described heterodyne reception of detector array 12 by described detector array 12 The acquired card 13 of signal described computer 14 of making a gift to someone carry out data processings.
Experiment shows that the present invention increases the optics toes and imaging vertically hung scroll of target face by way of multiple-input and multiple-output Degree, and the influence that the dutycycle in transmitting light path between the covering and fibre core of launching fiber is imaged to far field is considered, provide The inclination arrangement of optical fiber in fiber array device.In addition, for coherent detection system, field of view of receiver is by antenna law system About, Receiver aperture is inversely proportional with visual field.And in order to improve reception resolution ratio, reduce system power dissipation, it is often desirable that use heavy caliber Receive.In order to solve the contradiction between Receiver aperture and visual field, the present invention uses array heterodyne reception mode.This will be to remote High-resolution airbome synthetic aperture laser imaging radar has very important significance.

Claims (2)

1. a kind of multi-channel wide Amplitude Composition aperture laser imaging radar receive-transmit system, including emission system and reception system, its It is characterised by:
Described emission system includes LASER Light Source (1), frequency modulator (2), AWG (3), fiber optic splitter (4), fiber amplifier group (5), fiber array device (6), diversing lens (7), the first beam splitter (8) and Brewster prism shrink beam Device (9);
The output end of described LASER Light Source (1) is connected with the first input end of described frequency modulator (2), and described is any The output end of waveform generator (3) is connected with the second input of described frequency modulator (2), described frequency modulator (2) output end is connected with the input of described fiber optic splitter (4), the first output end of described fiber optic splitter (4), Second output end, the 3rd output end ..., the n-th output end puts with the first optical fiber in described fiber amplifier group (5) respectively The big input of device (51), the input of the second fiber amplifier (52), the 3rd fiber amplifier (53) input ..., The input of n-th fiber amplifier (5n) is connected, the first fiber amplifier (51) in described fiber amplifier group (5) it is defeated Go out end, the output end of the second fiber amplifier (52), the output end of the 3rd fiber amplifier (53) ..., the n-th fiber amplifier The output end of (5n) respectively the first input end with described fiber array device (6), the second input, the 3rd input ..., N-th input is connected, and the diversing lens (7) that the output light warp of described fiber array device (6) is described enter described first point Incident light is divided into transmitted light and reflected light, the described Bruce of described transmitted light warp by beam device (8), first beam splitter (8) Special prism shrink beam device (9) exports transmission signal, and described n is more than 3 positive integer;
Described reception system include receiving lens (10), the second beam splitter (11), detector array (12), capture card (13) and Computer (14);
The echo-signal that described transmission signal reflects through target face is successively through described receiving lens (10), through described Two beam splitters (11) simultaneously enter institute with the reflected light of described the first beam splitter (8) after described the second beam splitter (11) reflection The detector array (12) stated, the acquired card (13) of output end and the described computer (14) of described detector array (12) Input be connected.
2. multi-channel wide Amplitude Composition aperture laser imaging radar receive-transmit system according to claim 1, it is characterised in that: The diameter of every optical fiber in described fiber array device (6) is D, and core diameter is d, and the numbering of n root optical fiber is respectively: f1,f2,..,fn, the distance values dr that the cross rail of two adjacent optical fiber of subscript is upward is fixed, and is η times of core diameter, wherein, 0 < η < 1, the n root launching fibers in described fiber array device (6) are arranged in the following manner:
Keep tangent between adjacent two optical fiber, described launching fiber arrangement mode L is L=(f1,f2,..,fn), n root optical fiber Center line and horizontal line between angle theta meet following relation:
<mrow> <mi>sin</mi> <mi>&amp;theta;</mi> <mo>=</mo> <mfrac> <mrow> <mi>d</mi> <mi>r</mi> </mrow> <mi>D</mi> </mfrac> <mo>,</mo> </mrow>
The array element of described detector array (12) is identical with the quantity of the launching fiber of described fiber array device (6), arrangement Mode is consistent, closely coupled between each array element, and the angle theta between the line and horizontal line at the center of n array element meets as follows Relation:
<mrow> <mi>s</mi> <mi>i</mi> <mi>n</mi> <mi>&amp;theta;</mi> <mo>=</mo> <mfrac> <mrow> <mi>d</mi> <mi>r</mi> </mrow> <mi>D</mi> </mfrac> <mo>.</mo> </mrow>
CN201710828948.XA 2017-09-14 2017-09-14 Multi-channel wide-amplitude synthetic aperture laser imaging radar transmitting and receiving system Active CN107728130B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201710828948.XA CN107728130B (en) 2017-09-14 2017-09-14 Multi-channel wide-amplitude synthetic aperture laser imaging radar transmitting and receiving system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201710828948.XA CN107728130B (en) 2017-09-14 2017-09-14 Multi-channel wide-amplitude synthetic aperture laser imaging radar transmitting and receiving system

Publications (2)

Publication Number Publication Date
CN107728130A true CN107728130A (en) 2018-02-23
CN107728130B CN107728130B (en) 2020-10-16

Family

ID=61206266

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201710828948.XA Active CN107728130B (en) 2017-09-14 2017-09-14 Multi-channel wide-amplitude synthetic aperture laser imaging radar transmitting and receiving system

Country Status (1)

Country Link
CN (1) CN107728130B (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110346777A (en) * 2018-04-03 2019-10-18 通用汽车环球科技运作有限责任公司 Image intensifer in coherent lidar system return path
CN110346778A (en) * 2018-04-03 2019-10-18 通用汽车环球科技运作有限责任公司 Coherent lidar system with extended field of view
CN112213736A (en) * 2020-07-17 2021-01-12 中国工程物理研究院应用电子学研究所 Three-dimensional target imaging laser radar device and target detection method
WO2023061386A1 (en) * 2021-10-15 2023-04-20 华为技术有限公司 Laser radar, receiving system, emitting system, and control method
CN117805854A (en) * 2024-03-01 2024-04-02 中国科学院空天信息创新研究院 MIMO-based laser SAL wide-field imaging device and method

Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101630006A (en) * 2009-08-19 2010-01-20 中国科学院上海光学精密机械研究所 Lens focal plane array heterodyne reception optical antenna of synthetic aperture laser imaging radar
CN102215062A (en) * 2011-03-25 2011-10-12 中国科学院上海光学精密机械研究所 Multi-channel optical receiver system of synthetic aperture laser imaging radar
CN103018735A (en) * 2012-12-13 2013-04-03 中国科学院上海光学精密机械研究所 Synthetic aperture laser imaging radar large-visual-field heterodyne detection device
CN103885066A (en) * 2014-03-21 2014-06-25 中国科学院上海光学精密机械研究所 Synthetic aperture laser imaging radar bi-dimensional convolution imaging method
CN104570001A (en) * 2015-01-28 2015-04-29 中国科学院上海光学精密机械研究所 Synthetic aperture laser imaging radar optical processor based on band-pass filter
CN104965206A (en) * 2015-07-17 2015-10-07 中国科学院上海光学精密机械研究所 Phase encoding cross-polarization synthetic aperture laser imaging radar
EP2930532A1 (en) * 2014-04-09 2015-10-14 Raytheon Company Simultaneous forward and inverse synthetic aperture imaging ladar
CN105652285A (en) * 2016-01-12 2016-06-08 中国科学院上海光学精密机械研究所 Local oscillator enhanced reception device for direct-view synthetic aperture laser imaging radar
CN107102311A (en) * 2017-04-24 2017-08-29 中国科学院上海光学精密机械研究所 Orthoptic synthetic aperture laser imaging radar rotary reflection wavefront transformation scanning means

Patent Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101630006A (en) * 2009-08-19 2010-01-20 中国科学院上海光学精密机械研究所 Lens focal plane array heterodyne reception optical antenna of synthetic aperture laser imaging radar
CN102215062A (en) * 2011-03-25 2011-10-12 中国科学院上海光学精密机械研究所 Multi-channel optical receiver system of synthetic aperture laser imaging radar
CN103018735A (en) * 2012-12-13 2013-04-03 中国科学院上海光学精密机械研究所 Synthetic aperture laser imaging radar large-visual-field heterodyne detection device
CN103885066A (en) * 2014-03-21 2014-06-25 中国科学院上海光学精密机械研究所 Synthetic aperture laser imaging radar bi-dimensional convolution imaging method
EP2930532A1 (en) * 2014-04-09 2015-10-14 Raytheon Company Simultaneous forward and inverse synthetic aperture imaging ladar
CN104570001A (en) * 2015-01-28 2015-04-29 中国科学院上海光学精密机械研究所 Synthetic aperture laser imaging radar optical processor based on band-pass filter
CN104965206A (en) * 2015-07-17 2015-10-07 中国科学院上海光学精密机械研究所 Phase encoding cross-polarization synthetic aperture laser imaging radar
CN105652285A (en) * 2016-01-12 2016-06-08 中国科学院上海光学精密机械研究所 Local oscillator enhanced reception device for direct-view synthetic aperture laser imaging radar
CN107102311A (en) * 2017-04-24 2017-08-29 中国科学院上海光学精密机械研究所 Orthoptic synthetic aperture laser imaging radar rotary reflection wavefront transformation scanning means

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
JIN HE ET AL.: "Micro-Doppler Effect Analysis Based on Inverse Synthetic Aperture Imaging LADAR", 《IEEE 10TH INTERNATIONAL CONFERENCE ON SIGNAL PROCESSING PROCEEDINGS》 *
唐禹 等: "多发多收合成孔径激光雷达高分辨率宽测绘带成像", 《红外与激光工程》 *
孙志伟 等: "合成孔径激光成像雷达的光学成像处理", 《光学学报》 *

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110346777A (en) * 2018-04-03 2019-10-18 通用汽车环球科技运作有限责任公司 Image intensifer in coherent lidar system return path
CN110346778A (en) * 2018-04-03 2019-10-18 通用汽车环球科技运作有限责任公司 Coherent lidar system with extended field of view
CN110346778B (en) * 2018-04-03 2023-11-21 通用汽车环球科技运作有限责任公司 Coherent lidar system with extended field of view
CN110346777B (en) * 2018-04-03 2024-02-27 通用汽车环球科技运作有限责任公司 Optical amplifier in return path of coherent lidar system
CN112213736A (en) * 2020-07-17 2021-01-12 中国工程物理研究院应用电子学研究所 Three-dimensional target imaging laser radar device and target detection method
WO2023061386A1 (en) * 2021-10-15 2023-04-20 华为技术有限公司 Laser radar, receiving system, emitting system, and control method
CN117805854A (en) * 2024-03-01 2024-04-02 中国科学院空天信息创新研究院 MIMO-based laser SAL wide-field imaging device and method
CN117805854B (en) * 2024-03-01 2024-05-07 中国科学院空天信息创新研究院 MIMO-based laser SAL wide-field imaging device and method

Also Published As

Publication number Publication date
CN107728130B (en) 2020-10-16

Similar Documents

Publication Publication Date Title
CN107728130A (en) Multi-channel wide Amplitude Composition aperture laser imaging radar receive-transmit system
US11754681B2 (en) LIDAR system with a multi-mode waveguide photodetector
CN101408623B (en) Up-conversion imaging system of broad band synthetic aperture
CN101806625B (en) Static Fourier transform interference imaging spectrum full-polarization detector
CN105785343A (en) Spacial multi-beam laser emitter, multichannel receiving apparatus and detection apparatus
CN113841062B (en) LIDAR system with mode field expander
CN108574533A (en) A kind of Shared aperture laser communication optical transmitter and receiver based on optical phased array
US7639902B2 (en) Microwave photonic frequency domain reflectometer
CN101793558B (en) Device for detecting full polarization of passive and static coaxial interference imaging spectrum
CN104965206B (en) Cross-polarization is multiplexed synthetic aperture laser imaging radar
CN110456324A (en) Integrated phased-array laser radar system
CN101799327A (en) Passive static triangle common path interference imaging spectral full-polarization detecting device
CN107450179B (en) Active correlation imaging optical system based on multi-channel semiconductor laser
CN108710137A (en) Big visual field synthetic aperture laser imaging radar receive-transmit system
CN114839644A (en) Laser radar system
US9696212B2 (en) High efficiency coherent imager
CN108387974A (en) High-power optical fiber laser receiving and transmitting integrated end cap
CN109581411A (en) Synthetic aperture laser imaging radar receive-transmit system based on light beam optics coherence tomography
CN102004243A (en) Optical bridging heterodyne reception and complex value processing system for synthetic aperture laser imaging radar
CN106712846B (en) A kind of laser communication Optical devices adapting to different operating distance
CN114895281A (en) Method and device for generating target information by intrinsic signal and target return signal
CN110186568B (en) Photon mixing terahertz wave detection device
CN207924208U (en) Light transmit-receive integrated optical device is realized under co-wavelength
CN103163532B (en) Wide-scroll direct vision synthetic aperture laser imaging radar
CN106342249B (en) Laser synthetic aperture imaging system

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
TR01 Transfer of patent right
TR01 Transfer of patent right

Effective date of registration: 20221102

Address after: 215638 310A, Building B, Science and Technology Innovation Park, Zhangjiagang Free Trade Zone, Suzhou, Jiangsu Province

Patentee after: Suzhou Xuanguang Semiconductor Technology Co.,Ltd.

Address before: 201800 Qinghe Road 390, Shanghai, Jiading District

Patentee before: SHANGHAI INSTITUTE OF OPTICS AND FINE MECHANICS CHINESE ACADEMY OF SCIENCES