CN106444056A - Sparse optical synthetic aperture imaging device based on three apertures and light beam combination correction method of device - Google Patents

Sparse optical synthetic aperture imaging device based on three apertures and light beam combination correction method of device Download PDF

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CN106444056A
CN106444056A CN201611126713.8A CN201611126713A CN106444056A CN 106444056 A CN106444056 A CN 106444056A CN 201611126713 A CN201611126713 A CN 201611126713A CN 106444056 A CN106444056 A CN 106444056A
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imaging
corner cube
prism
light
device based
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CN106444056B (en
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马浩统
谢宗良
亓波
任戈
史建亮
董理
崔占刚
刘欣诚
陈丰
张美丽
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Institute of Optics and Electronics of CAS
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    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/10Beam splitting or combining systems
    • G02B27/108Beam splitting or combining systems for sampling a portion of a beam or combining a small beam in a larger one, e.g. wherein the area ratio or power ratio of the divided beams significantly differs from unity, without spectral selectivity
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/0025Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 for optical correction, e.g. distorsion, aberration

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  • Optics & Photonics (AREA)
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Abstract

The invention discloses a sparse optical synthetic aperture imaging device based on three apertures and a light beam combination correction method of the device. The device and the method can be used for remarkably improving the imaging resolving power of a target and effectively weakening the influence of transmission media such as atmosphere and optical systems. The device mainly comprises a telescope sub-array, an optical distance precision adjustment system, an oblique error correction unit, an imaging light sub-beam combination and imaging system and the like. After light waves reflected or scattered by the target are respectively acquired by the telescope sub-array, three imaging light waves share a phase by the aid of the optical distance precision adjustment system and the oblique error correction unit, and finally, high-resolution synthetic aperture imaging for the target is realized by the imaging light sub-beam combination and imaging system. The device has the advantages of simple and compact structure, small size, light weight, high environmental adaptability, capability of simultaneously ensuring optical distance precision adjustment range and adjustment accuracy and the like.

Description

A kind of sparse optical synthesis aperture imaging device based on three apertures and its light beam close bundle Bearing calibration
Technical field
The invention belongs to optical technical field, and in particular to a kind of sparse optical synthesis aperture imaging dress based on three apertures Put and its light beam closes beam alignment method.
Background technology
The continuous development and progress of science and technology, many necks such as imaging, military surveillance, astronomical observation and survey of deep space over the ground Higher and higher resolution is needed in domain.For the single port footpath optical system for commonly using at present, in order to improve spatial resolution Certainly will to increase system bore, but the increase of system bore is subject to material, technique, manufacturing cost, quality and payload bay The restriction of the factors such as volume, while also inevitably result in the volume of system and quality increase, to space base and spacebased system Transmitting brings difficulty.Synthesis aperture imaging system is made up of some rim of the mouth footpath imaging systems for being arranged into specific array form, per The light beam of individual sub- bore is transmitted to beam synthesis after phase adjustment, and interference imaging on confocal face.Due to itself Caused by system structure feature and imaging mode, synthesis aperture imaging system is compared single aperture imaging system and is obtained in that target is more Radio-frequency component, so as to effectively improve imaging observation precision, detect the more fine structures of target, realize equivalent single macropore The resolution capability of footpath imaging system.
Synthetic aperture imaging technology is generally divided into two kinds:Baseline interference synthetic aperture technology and sparse optical synthesis aperture skill Art.Complex degree of coherence is obtained compared to baseline interference synthetic aperture technology by inverting interference fringe to be imaged, sparse optics synthesis Aperture technique is then that multiple sub-aperture of utilization space particular arrangement are directly synthesized to target imaging, with sufficient motility, Dynamic object is more conducively directly observed.The correlation theory of sparse optical synthesis aperture imaging system and technical research are always the world Study hotspot, it is in other imaging techniques such as ground and space-based Large Telescope System, Laser Transmission, micro-imaging, three-dimensional imaging Field has a wide range of applications.Carry out related research, set up the synthetic aperture of simple and compact for structure, small in volume Imaging system has important scientific meaning and application prospect.
Content of the invention
Present invention aim in view of the shortcomings of the prior art, a kind of sparse optics based on three apertures is provided and is synthesized Aperture imaging device and its light beam close beam alignment method.The present invention mainly by sub- telescope array, light path fine adjustment system, incline Oblique error corrects unit, closes the composition such as bundle and imaging system.The present invention has simple and compact for structure, small in volume, environment Adaptable, the advantages of light path range of accommodation and degree of regulation can be ensured simultaneously, space-based, space base etc. to the weight of platform and Volume has in the applied environment of strict demand, with obvious advantage.
The technical solution of the present invention is:
1.. a kind of sparse optical synthesis aperture imaging device based on three apertures, structure is as shown in figure 1, Cassegrain hopes Remote mirror 1 and collimating lens 2 constitute sub- telescope array, and high-precision large-stroke combines displacement platform and is fixed thereon the pyramid rib in face Mirror 3 constitutes light path fine adjustment system, and anti-mirror 4 is tilt corrector unit soon, and outer surface is the corner cube reflector 5 of reflecting surface, becomes As lens 6 and the composition of CCD camera 7 close bundle and imaging system.The light wave of target reflection or scattering is penetrated after sub- telescope array Entering prism of corner cube 3, the imaging light wave that returns is turned back after the reflection of anti-mirror 4 soon, by corner cube reflector and imaging len, image in CCD camera 7.Light path fine adjustment system and tilt corrector unit cause each road imaging light wave common phase position, realize to target High-resolution synthetic aperture imaging, image-forming principle is Fizeau interference principle.
The image that CCD is collected is:
I (x, y)=o (x, y) * h (x, y)+n (x, y)
In formula, o (x, y) is point spread function of preferable several picture, the h (x, y) for system, and n (x, y) is CCD camera Noise, (x, y) represents convolution for the coordinate vector of image plane, *.Point spread function h (x, y) of system can be characterized as:
P in formulak(u, v) is the pupil function of subsystem, Zm(u, v) is zernike polynomial, and m=1 represents the flat of sub-aperture Shift error, m=2 and m=3 represent the heeling error in two mutually perpendicular directions, α respectivelymFor corresponding coefficient,Table Show Fourier transformation.According to the translation for measuring and heeling error, error system is made by light path fine adjustment and tilt correction system Number αm0 is approximately, the common phase position of each road imaging beam is can achieve, and obtains the high-resolution composograph of target.
2.. light path fine adjustment mainly combines displacement platform by high-precision large-stroke and is fixed thereon the prism of corner cube 3 in face Realize.Prism of corner cube causes imaging beam original road to turn back, and the present invention is synthesized into by the position of accurate mobile prism of corner cube, correction As the translation error between each road of system.High-precision large-stroke precision displacement table is by the low Accuracy Displacement platform 9 of big stroke and little stroke height Accuracy Displacement platform 8 is combined.
3.. the two-dimensional deflection of light beam realized by the controlled anti-soon mirror 4 of programming, can quickly correct each sub-aperture incident imaging light The inclined aberration of ripple so that three road imaging beams are imaged at the same position of CCD.
4.. close the conjunction bundle that bundle and the corner cube reflector 5 in imaging system realize three road imaging beams.It is different from light path precision Prism of corner cube in regulating system, corner cube reflector 5 is processed through particular design as bundling device, its three cone outer surface use In the reflected beams, the three road imaging beams that subsystem is transmitted close bundle and shine on imaging len, then are realized by main lenss Compound imaging.Corner cube reflector 5 is fixed on an accurate translation stage, for controlling relative position of outgoing imaging beam etc., It is imaged, to ensure that emergent pupil and entrance pupil meet Fizeau interference, " golden ratio " that need to follow.
Wherein, the device realizes light beam compound imaging by three way telescopic systems, is a kind of phased telescope array.Become As principle is Fizeau interference principle, directly can to carry out high-resolution compound imaging to target.
Wherein, light path is turned back by light path fine adjustment system using prism of corner cube, makes whole system more simply compact, while Reduce the weight and volume of system.Realized using the low Accuracy Displacement platform of big stroke and the cascade of little stroke and high precision displacement platform high-precision Big stroke positioning is spent, the modification scope of light path had both been ensure that, also ensure that the degree of regulation of light path.
Wherein, three soon anti-mirror realize the deflection of light beam, correct the heeling error of system.
Wherein, closing bundle imaging system the corner cube reflector using axicon lens outer surface as reflecting surface of particular design is used as conjunction Bundle device, while corner cube reflector is fixed on accurate translation stage, need to be followed with ensureing that emergent pupil and entrance pupil meet Fizeau interference imaging " golden ratio ".
The present invention compared with prior art, has the advantage that:
1. compared with single aperture imaging system, imaging device proposed by the present invention, directly target object can be carried out more The imaging of high resolution.After light path fine adjustment and tilt correction system eliminate the common phase error of subsystems, 3 prestiges Remote mirror system can be equivalent to a heavy caliber system, so as to effectively improve the resolution of imaging system.Single aperture is imaged Respectively as shown in Figure 3 and Figure 4, compound imaging effectively can be carried the Numerical Simulation Results being imaged with three aperture synthetic as seen from the figure High imaging resolution capability.
2., compared with other sparse optical synthesis aperture imaging devices, imaging device proposed by the present invention, using height essence The cascade of degree translation stage is adjusted with the high-precision large-stroke for realizing each road imaging beam light path, is ensureing the same of light path degree of regulation When, it is possible to obtain bigger modification scope.While the correction that realizes inclining using anti-mirror soon, translation stage and soon anti-mirror are all programmed can Control, it is possible to achieve the quick common phase closed loop control of system.
3. compared with other sparse optical synthesis aperture imaging devices, imaging device proposed by the present invention, simple structure, special Be not using prism of corner cube, anti-mirror and corner cube reflector etc. soon, so that compound imaging is completed in the space of light beam incidence, so as to allow Whole system structure is compacter, and the volume and weight of system is reduced further.
Description of the drawings
Fig. 1 is the sparse optical synthesis aperture imaging device schematic diagram based on three apertures proposed by the present invention, wherein, Fig. 1 A () is horizontal double-barrel structure top view, Fig. 1 (b) is top monotubular structural side view;
Fig. 2 combines displacement platform schematic diagram for high-precision large-stroke proposed by the present invention;
Fig. 3 is compound imaging system single aperture imaging point spread function and the imaging point spread function signal of three aperture synthetic Figure, wherein, it is three aperture point spread function schematic diagrams that Fig. 3 (a) is single aperture point spread function schematic diagram, Fig. 3 (b);
Fig. 4 is compound imaging system single aperture image and three aperture synthetic image schematic diagrams, wherein, Fig. 4 (a) For single aperture image schematic diagram, Fig. 4 (b) is three aperture synthetic image schematic diagrams.
In figure reference implication is:1 is Cassegrain telescope, and 2 is collimating lens, and 3 is prism of corner cube, and 4 is fast anti- Mirror, 5 is corner cube reflector, and 6 is imaging len, and 7 is CCD camera.
Specific embodiment
Below in conjunction with the accompanying drawings and specific embodiment further illustrates the present invention.
The structure of whole imaging device is as shown in figure 1, mainly including look in the distance mirror system, light path fine adjustment system, incline Tiltedly correction system, light beam close bundle and imaging system.Cassegrain telescope 1 and collimating lens 2 constitute mirror system of looking in the distance, fixing Prism of corner cube 3 on the large stroke and high precision displacement platform for being cascaded by height precision translation stage 8 and 9 is light path fine adjustment system System, anti-mirror 4 is tilt correction system soon, and outer surface is that corner cube reflector 5, imaging len 6 and the CCD camera 7 of reflecting surface constitute Imaging beam closes bundle and imaging system.
Its specific work process is:
1. mirror system of looking in the distance receives the imaging light wave of target object reflection or scattering respectively, obtains three tunnels and does not correct altogether The subsystem imaging beam of phase error.After three road imaging beams are turned back by prism of corner cube, pyramid reflection is reflexed to through too fast anti-mirror On the reflecting surface of mirror, after reflected face reflection, realize closing bundle.The accurate position for adjusting the reflection angle of anti-mirror and corner cube reflector soon Put, be imaged, to ensure that emergent pupil and entrance pupil meet Fizeau interference, " golden ratio " that need to follow.Light beams are closed after imaging len Image in above CCD camera.CCD camera collection light distribution now.
2. according to the intensity signal of CCD collection, using the common phase algorithm that some have been reported, such as far-field spot detection, out of focus Phase difference method, shutter phase difference method, neutral net etc., detect the common phase errors such as translation and inclination between subsystem.To visit The error signal for obtaining is input in light path fine adjustment and tilt correction system, is compensated accordingly, to eliminate son as feedback Common phase error between system, realizes the common phase position of each subsystem light beam, directly obtains high-resolution synthetic aperture on CCD Image.
The above is only the preferred embodiment of the present invention, and protection scope of the present invention is not limited to above-mentioned enforcement Example, all designs for belonging under thinking of the present invention belong to protection scope of the present invention.It should be pointed out that for the art Those of ordinary skill for, some improvements and modifications without departing from the principles of the present invention, these retouchings and improve Should be regarded as protection scope of the present invention.

Claims (9)

1. a kind of sparse optical synthesis aperture imaging device based on three apertures, it is characterised in that:Including Cassegrain telescope (1), collimating lens (2), prism of corner cube (3), anti-mirror (4) soon, corner cube reflector (5), imaging len (6), CCD camera (7), its In,
Cassegrain telescope (1) and collimating lens (2) constitute sub- telescope array, and high-precision large-stroke combines displacement platform and consolidates Prism of corner cube (3) above which constitutes light path fine adjustment system, and anti-mirror (4) soon is tilt corrector unit, and outer surface is The corner cube reflector (5) of reflecting surface, imaging len (6) and CCD camera (7) are constituted closes bundle and imaging system, target reflection or The light wave of scattering injects prism of corner cube (3) after sub- telescope array, and the imaging light wave that returns of turning back is through anti-mirror (4) reflection soon Afterwards, by corner cube reflector and imaging len, CCD camera (7) is imaged in, light path fine adjustment system and tilt corrector unit make Obtain each road and light wave common phase position is imaged, realize the high-resolution synthetic aperture imaging to target.
2. the sparse optical synthesis aperture imaging device based on three apertures according to claim 1, it is characterised in that:The dress Put and realize imaging beam compound imaging by three way telescopes, be a kind of phased telescope array, the size of aperture of mirror of looking in the distance and Arrangement can be designed according to the actual requirements.
3. the sparse optical synthesis aperture imaging device based on three apertures according to claim 1, it is characterised in that:Use Prism of corner cube by each road imaging beamlet turn back so that whole system is simple and compact for structure, at the same reduce system weight and Volume.
4. the sparse optical synthesis aperture imaging device based on three apertures according to claim 1, it is characterised in that:Its light Journey fine adjustment mainly combines displacement platform by high-precision large-stroke and is fixed thereon prism of corner cube (3) realization in face;In high precision Big travel displacement platform is mainly made up of the low Accuracy Displacement platform of big stroke and the cascade of little stroke and high precision displacement platform.
5. the sparse optical synthesis aperture imaging device based on three apertures according to claim 1, it is characterised in that:Use Three soon anti-mirror realize the deflection of light beam, correct the heeling error of system.
6. the sparse optical synthesis aperture imaging device based on three apertures according to claim 1, it is characterised in that:Use The corner cube reflector using axicon lens outer surface as reflecting surface of particular design as bundling device, while corner cube reflector is fixed on precision On translation stage, for controlling relative position of outgoing imaging beam etc., need are imaged to ensure that emergent pupil and entrance pupil meet Fizeau interference " golden ratio " for following, in actual applications, corner cube reflector can also adopt three pieces of reflecting mirrors to constitute pyramidal structure come real The conjunction bundle of existing imaging beam.
7. the sparse optical synthesis aperture imaging device based on three apertures according to claim 1, it is characterised in that:The dress The image-forming principle that puts is Fizeau interference principle, directly can carry out high-resolution compound imaging to target.
8. the sparse optical synthesis aperture imaging device based on three apertures according to claim 1, it is characterised in that:It is based on The comprehensive translation error for realizing each road imaging beam such as prism of corner cube, fast mirror and corner cube reflector and heeling error correction And imaging beam closes bundle, simple and compact for structure.
9. a kind of sparse optical synthesis aperture imaging device based on three apertures carries out the method that light beam closes beam alignment, using right Require the device described in 1, it is characterised in that:The method comprises the steps:
1. the image that .CCD is collected is:
I (x, y)=o (x, y) * h (x, y)+n (x, y)
In formula, o (x, y) is point spread function of preferable several picture, the h (x, y) for system, and n (x, y) is made an uproar for CCD camera Sound, (x, y) represents convolution for the coordinate vector of image plane, *, and point spread function h (x, y) of system can be characterized as:
P in formulak(u, v) is the pupil function of sub- telescope, Zm(u, v) is zernike polynomial, and m=1 represents the translation of sub-aperture Error, m=2 and m=3 represent the heeling error in two mutually perpendicular directions, α respectivelymFor corresponding coefficient,Represent Fourier transformation, according to the translation for measuring and heeling error, makes error coefficient by light path fine adjustment and tilt correction system αm0 is approximately, the common phase position of each road imaging beam is can achieve, and obtains the high-resolution composograph of target;
2.. light path fine adjustment mainly combines displacement platform by high-precision large-stroke and is fixed thereon prism of corner cube (3) reality in face Existing, prism of corner cube causes imaging beam original road to turn back, and by the position of accurate mobile prism of corner cube, correction compound imaging system is each Translation error between road, high-precision large-stroke precision displacement table is by big stroke low Accuracy Displacement platform (9) and little stroke and high precision position Moving stage (8) cascading is formed;
3.. the two-dimensional deflection of light beam is realized in programming controlled anti-soon mirror (4), can quickly correct each sub-aperture incident imaging light ripple Inclined aberration so that three road imaging beams are imaged at the same position of CCD;
4.. close the conjunction bundle that bundle and the corner cube reflector (5) in imaging system realize three road imaging beams;It is different from the accurate tune of light path Prism of corner cube in section system, corner cube reflector (5) is used as bundling device, and its three cone outer surfaces are used for the reflected beams, by subsystem The three road imaging beams that system is transmitted close bundle and shine on imaging len, then realize compound imaging by main lenss, and pyramid reflects Mirror (5) is fixed on an accurate translation stage, for controlling relative position of outgoing imaging beam etc., to ensure emergent pupil and entrance pupil Meet " golden ratio " that Fizeau interference imaging need to be followed.
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Cited By (13)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107450176A (en) * 2017-09-21 2017-12-08 中国科学院上海天文台 A kind of space sparse aperture telescope common phase control device and control method
CN108955640A (en) * 2018-04-23 2018-12-07 中国科学院光电技术研究所 The restructural remote sensing camera in space based on synthetic aperture technique
CN109029925A (en) * 2018-06-12 2018-12-18 中国科学院上海技术物理研究所 It is a kind of for aim at monitoring telescope optic axis block prism light calibration device
CN109946711A (en) * 2019-03-29 2019-06-28 西安电子科技大学 The flexible synthetic aperture optical imagery pilot system with rotation of baseline
CN110646947A (en) * 2019-09-11 2020-01-03 中国科学院光电技术研究所 Pupil space modulation device and method
CN110771135A (en) * 2017-04-13 2020-02-07 弗劳恩霍夫应用研究促进协会 Multi-aperture image forming apparatus, image forming system, and method of providing multi-aperture image forming apparatus
CN110771132A (en) * 2017-05-23 2020-02-07 弗劳恩霍夫应用研究促进协会 Multi-aperture imaging device, imaging system, and method for providing a multi-aperture imaging device
CN111638040A (en) * 2020-05-14 2020-09-08 中国科学院光电技术研究所 Defocusing decoupling pointing correction method suitable for optical synthetic aperture imaging system
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CN113534436A (en) * 2021-07-09 2021-10-22 西安工业大学 Sparse synthetic aperture imaging system based on seven apertures and phase correction method thereof

Citations (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5159489A (en) * 1990-05-16 1992-10-27 The United States Of America As Represented By The United States Department Of Energy High resolution telescope
CN1632642A (en) * 2004-12-13 2005-06-29 中国科学院上海技术物理研究所 Correction method for registration of infrared rear optical system optical axis and system axis of remote sensing instrument
CN1908722A (en) * 2006-08-17 2007-02-07 中国科学院光电技术研究所 High resolution imaging self-adaptive optical telescope suitable for working at daytime
CN102073147A (en) * 2010-12-23 2011-05-25 中国科学院西安光学精密机械研究所 Multi-telescope optical synthetic aperture imaging system and design method thereof
CN102122082A (en) * 2011-03-23 2011-07-13 中国科学院光电技术研究所 Phase shift error correction device for sparse optical synthetic aperture imaging system
CN103128731A (en) * 2013-03-14 2013-06-05 中国科学院自动化研究所 Micro-assembly robot system
CN204575985U (en) * 2015-05-14 2015-08-19 中国船舶重工集团公司第七一七研究所 A kind of sparse synthetic aperture optical imaging device with four apertures
CN104898108A (en) * 2015-05-19 2015-09-09 浙江大学 Atmosphere remote sensing laser radar optical receiving device based on telescope arrays
CN105115427A (en) * 2015-09-16 2015-12-02 中国科学院光电技术研究所 Method for improving anti-noise capability of dispersed fringe sensor co-phasing system
CN105824030A (en) * 2016-03-10 2016-08-03 中国科学院光电技术研究所 Sparse optical synthetic aperture imaging method based on subaperture shutter modulation phase difference method

Patent Citations (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5159489A (en) * 1990-05-16 1992-10-27 The United States Of America As Represented By The United States Department Of Energy High resolution telescope
CN1632642A (en) * 2004-12-13 2005-06-29 中国科学院上海技术物理研究所 Correction method for registration of infrared rear optical system optical axis and system axis of remote sensing instrument
CN1908722A (en) * 2006-08-17 2007-02-07 中国科学院光电技术研究所 High resolution imaging self-adaptive optical telescope suitable for working at daytime
CN102073147A (en) * 2010-12-23 2011-05-25 中国科学院西安光学精密机械研究所 Multi-telescope optical synthetic aperture imaging system and design method thereof
CN102122082A (en) * 2011-03-23 2011-07-13 中国科学院光电技术研究所 Phase shift error correction device for sparse optical synthetic aperture imaging system
CN103128731A (en) * 2013-03-14 2013-06-05 中国科学院自动化研究所 Micro-assembly robot system
CN204575985U (en) * 2015-05-14 2015-08-19 中国船舶重工集团公司第七一七研究所 A kind of sparse synthetic aperture optical imaging device with four apertures
CN104898108A (en) * 2015-05-19 2015-09-09 浙江大学 Atmosphere remote sensing laser radar optical receiving device based on telescope arrays
CN105115427A (en) * 2015-09-16 2015-12-02 中国科学院光电技术研究所 Method for improving anti-noise capability of dispersed fringe sensor co-phasing system
CN105824030A (en) * 2016-03-10 2016-08-03 中国科学院光电技术研究所 Sparse optical synthetic aperture imaging method based on subaperture shutter modulation phase difference method

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
于树海: "傅里叶望远镜成像关键技术研究", 《中国优秀博士学位论文全文数据库工程科技Ⅱ辑》 *
李景镇 主编: "《光学手册 下卷》", 31 July 2010, 陕西科学技术出版社 *
黄一帆 等编著: "《光学设计教程》", 30 November 2009, 北京理工大学出版社 *

Cited By (22)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110771135B (en) * 2017-04-13 2022-06-07 弗劳恩霍夫应用研究促进协会 Multi-aperture image forming apparatus, image forming system, and method of providing multi-aperture image forming apparatus
CN110771135A (en) * 2017-04-13 2020-02-07 弗劳恩霍夫应用研究促进协会 Multi-aperture image forming apparatus, image forming system, and method of providing multi-aperture image forming apparatus
CN110771132A (en) * 2017-05-23 2020-02-07 弗劳恩霍夫应用研究促进协会 Multi-aperture imaging device, imaging system, and method for providing a multi-aperture imaging device
CN110771132B (en) * 2017-05-23 2022-04-26 弗劳恩霍夫应用研究促进协会 Multi-aperture imaging apparatus and method for providing a multi-aperture imaging apparatus
US11106047B2 (en) 2017-05-23 2021-08-31 Fraunhofer-Gesellschaft zur Förderung der angewandten Forschung e.V. Multi-aperture imaging device, imaging system and method for providing a multi-aperture imaging device
CN107450176A (en) * 2017-09-21 2017-12-08 中国科学院上海天文台 A kind of space sparse aperture telescope common phase control device and control method
CN108955640A (en) * 2018-04-23 2018-12-07 中国科学院光电技术研究所 The restructural remote sensing camera in space based on synthetic aperture technique
CN109029925A (en) * 2018-06-12 2018-12-18 中国科学院上海技术物理研究所 It is a kind of for aim at monitoring telescope optic axis block prism light calibration device
CN109029925B (en) * 2018-06-12 2023-12-26 中国科学院上海技术物理研究所 Cubic prism optical correction device for sighting and monitoring telescope optical axis
CN109946711B (en) * 2019-03-29 2021-03-12 西安电子科技大学 Synthetic aperture optical imaging test system with telescopic and rotary base line
CN109946711A (en) * 2019-03-29 2019-06-28 西安电子科技大学 The flexible synthetic aperture optical imagery pilot system with rotation of baseline
CN110646947B (en) * 2019-09-11 2021-08-13 中国科学院光电技术研究所 Pupil space modulation device and method
CN110646947A (en) * 2019-09-11 2020-01-03 中国科学院光电技术研究所 Pupil space modulation device and method
CN111638040B (en) * 2020-05-14 2022-04-19 中国科学院光电技术研究所 Defocusing decoupling pointing correction method suitable for optical synthetic aperture imaging system
CN111638040A (en) * 2020-05-14 2020-09-08 中国科学院光电技术研究所 Defocusing decoupling pointing correction method suitable for optical synthetic aperture imaging system
CN112230367A (en) * 2020-09-29 2021-01-15 四川大学 Accurate light beam converging device, light beam regulating and controlling method and sparse aperture imaging system
CN112230441A (en) * 2020-09-29 2021-01-15 四川大学 Debugging device and method for sparse aperture imaging system
CN112764236A (en) * 2021-01-21 2021-05-07 湖北航天技术研究院总体设计所 Array light beam emission and imaging integrated device, system and use method
CN112764236B (en) * 2021-01-21 2022-04-29 湖北航天技术研究院总体设计所 Array light beam emission and imaging integrated device, system and use method
CN113536655A (en) * 2021-04-07 2021-10-22 北京聚树核科技有限公司 Artificial intelligent deviation rectifying method and device for heliostat, electronic equipment and storage medium
CN113536655B (en) * 2021-04-07 2022-07-22 北京聚树核科技有限公司 Heliostat artificial intelligence deviation rectifying method, heliostat artificial intelligence deviation rectifying device, electronic equipment and storage medium
CN113534436A (en) * 2021-07-09 2021-10-22 西安工业大学 Sparse synthetic aperture imaging system based on seven apertures and phase correction method thereof

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