CN107966277A - Nearly back-scattering light time measurement system based on ellipsoid diffusing reflection blank - Google Patents

Nearly back-scattering light time measurement system based on ellipsoid diffusing reflection blank Download PDF

Info

Publication number
CN107966277A
CN107966277A CN201711341523.2A CN201711341523A CN107966277A CN 107966277 A CN107966277 A CN 107966277A CN 201711341523 A CN201711341523 A CN 201711341523A CN 107966277 A CN107966277 A CN 107966277A
Authority
CN
China
Prior art keywords
ellipsoid
diffusing reflection
time measurement
shortwave
long wave
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
CN201711341523.2A
Other languages
Chinese (zh)
Other versions
CN107966277B (en
Inventor
闫亚东
何俊华
张敏
韦明智
薛艳博
许瑞华
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.)
XiAn Institute of Optics and Precision Mechanics of CAS
Original Assignee
XiAn Institute of Optics and Precision 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 XiAn Institute of Optics and Precision Mechanics of CAS filed Critical XiAn Institute of Optics and Precision Mechanics of CAS
Priority to CN201711341523.2A priority Critical patent/CN107966277B/en
Publication of CN107966277A publication Critical patent/CN107966277A/en
Application granted granted Critical
Publication of CN107966277B publication Critical patent/CN107966277B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01MTESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
    • G01M11/00Testing of optical apparatus; Testing structures by optical methods not otherwise provided for
    • G01M11/02Testing optical properties
    • G01M11/0207Details of measuring devices
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02ATECHNOLOGIES FOR ADAPTATION TO CLIMATE CHANGE
    • Y02A90/00Technologies having an indirect contribution to adaptation to climate change
    • Y02A90/10Information and communication technologies [ICT] supporting adaptation to climate change, e.g. for weather forecasting or climate simulation

Abstract

The invention belongs to field of optical measuring technologies, and in particular to a kind of nearly back-scattering light time measurement system based on ellipsoid diffusing reflection blank.The measuring system includes sampler and measuring device, and sampler includes spherical vacuum target chamber and sampling diaphragm, target spot and ellipsoid diffusing reflection blank are provided with spherical vacuum target chamber;The nearly back-scattering light that target practice laser light incident target spot produces produces diffusing reflection along after the scattering of target practice opposite direction by ellipsoid diffusing reflection blank, enters measuring device after the sampled diaphragm sampling that diffuses;Target spot is located in a focus of ellipsoid diffusing reflection blank, and sampling diaphragm center is located in another focus of ellipsoid diffusing reflection blank.The present invention is using the diffusing reflection blank with ellipsoid type as scattering surface, eliminate the system time error introduced by scattering surface diffusing reflection, the temporal resolution of nearly backscattering time measurement system is improved, realizes the zero-time tolerance design of scattering time optical path.

Description

Nearly back-scattering light time measurement system based on ellipsoid diffusing reflection blank
Technical field
The invention belongs to field of optical measuring technologies, and in particular to a kind of near backwards to scattered based on ellipsoid diffusing reflection blank Penetrate light time measurement system.
Background technology
Laser fusion is a kind of human controllable's nuclear fusion generally used at present, it all has ten on civilian and military Divide great research significance:A kind of inexhaustible Clear nuclear energy source is explored for the mankind;For developing " clean ", (no radiation is dirty Dye) nuclear weapon, development high energy laser weapon;Part substitutes nuclear tests.
Therefore, laser fusion is paid much attention to be subject to each nuclear power of the world, since second half the 1970s, The states such as Russia, U.S., day, method, China and British start the development of high-power laser driver in succession.Research of the U.S. in this field is in neck First status, and formally built up the ultra-large type laser driving apparatus " NIF " comprising 192 tunnels in 2009;The MLF that France is building Include 240 road laser;Construction large laser driver is also fermenting in Japan, and plans to complete to apply between 2015-2020 In the basic technology research of power generation.China also establishes a series of laser driving apparatus (starlight series, God Light series etc.), The laser driving apparatus " Shenguang-Ⅲ " of the largest domestic for completing to build in 2015 includes 48 road laser.
However, U.S. NIF did not succeed in the igniting of 2010, this causes larger shock in world wide.NIF with Research afterwards finds that the theoretical model verified originally on small-scale laser driver is no longer applicable on NIF, and NIF practices shooting The backscattering share of laser is well beyond original desired value, and target practice laser energy is significantly slackened, fusion fuel compression Symmetry is destroyed, and causes loss of ignition, it can be seen that backscattering measuring system is in one new Laser Driven dress of understanding The irreplaceable effect played during putting.
The domestic research starting to backscattering is also relatively early, and the development of backscattering diagnostic techniques substantially experienced three ranks Section:
First stage, is measured after being sampled using glass spherical mirror to nearly back-scattering light, but the thing of the program, mirror body Normal direction, as three necessarily be on straight line, this arrangement mode is excessively stiff, without flexibility;
Second stage, is measured after being focused on using aluminum off-axis ellipsoidal mirror to nearly back-scattering light, by adjusting off-axis The achievable any light path layout of amount, flexibility ratio are very big, and focusing is very good, but the laser damage threshold of metallic mirror surface is relatively low (it is less than 1J/cm2), using limited on more extensive laser driving apparatus;
Phase III, using standard white plate of diffuse reflectance to nearly back-scattering light diffusing reflection, to being measured after the sampling that diffuses, The laser damage threshold of diffusing reflection blank (is more than 1.7J/cm2) it disclosure satisfy that the measurement demand of more extensive laser driving apparatus. But when carrying out nearly backscattering time measurement after to the sampling that diffuses, due to each point on plane diffusing reflection blank The light path of the measurements of arrival time that diffuses probe is different, and there are the different degrees of time difference (plane of 2m × 2m between each other Diffusing reflection plate maximum time difference is up to ns magnitudes, and backscattering time course to be measured is also several ns), time measurement system will be become The Systematic Errors of system, seriously reduce the temporal resolution of time measurement system.
The content of the invention
It is an object of the present invention to provide a kind of nearly back-scattering light time measurement system based on ellipsoid diffusing reflection blank, solution Determine the technical problem that systematic error is big, temporal resolution is low existing for existing nearly back-scattering light time measurement system.
The present invention technical solution be:A kind of nearly back-scattering light time measurement based on ellipsoid diffusing reflection blank System, including sampler and measuring device, it is characterized in that:The sampler includes spherical vacuum target chamber and sampling Diaphragm, is provided with target spot and ellipsoid diffusing reflection blank in the spherical vacuum target chamber;Target practice laser light incident target spot produces near Back-scattering light produces diffusing reflection along after the scattering of target practice opposite direction by ellipsoid diffusing reflection blank, and the sampled diaphragm that diffuses takes Enter measuring device after sample;The target spot is located in a focus of ellipsoid diffusing reflection blank, the sampling diaphragm centre bit In in another focus of ellipsoid diffusing reflection blank.
Further, above-mentioned measuring device includes imaging lens, the shrink beam positive lens set gradually along paths direction And dichroscope;After the dichroscope separates spectrum, long wave is transmitted anti-into long wave transmission light measurements unit, shortwave Inject into shortwave reflected light measurement unit.
It is preferred that above-mentioned long wave transmission light measurements unit includes long wave time measurement coupling mirror and the fast light of long wave time measurement Fulgurite;Long wave transmitted light samples light as the long wave where long wave time measurement coupling mirror images in the fast photoelectric tube of long wave time measurement In late image planes.
Further, it is provided with long wave light absorbs trap in above-mentioned long wave sampling diaphragm image planes.
Further, long wave spectrum sampling optical fiber is additionally provided with above-mentioned long wave sampling diaphragm image planes.
It is preferred that above-mentioned shortwave reflected light measurement unit includes shortwave time measurement coupling mirror and the fast light of shortwave time measurement Fulgurite;Shortwave reflected light samples light as the shortwave where shortwave time measurement coupling mirror images in the fast photoelectric tube of shortwave time measurement In late image planes.
Further, it is provided with short wavelength light absorption trap in above-mentioned shortwave sampling diaphragm image planes.
Further, shortwave spectrum sampling optical fiber is additionally provided with above-mentioned shortwave sampling diaphragm image planes.
It is preferred that above-mentioned imaging lens image in ellipsoid diffusing reflection blank in image planes, in an image planes It is provided with veiling glare filter.
The beneficial effects of the present invention are:
(1) present invention is eliminated because of scattering surface diffusing reflection using the diffusing reflection blank with ellipsoid type as scattering surface The system time error of introducing, improves the temporal resolution of nearly backscattering time measurement system, realizes scattering time survey Measure the zero-time tolerance design of light path.
(2) by the sampling of sampler acquisition, just each point is overflow the present invention on the diffusing reflection face of ellipsoid type diffusing reflection blank The aggregate of reflected light, 100% all standing is realized in time measurement test surface using the mode of Image relaying by stop imagery Sampling, measurement result are truer.
Brief description of the drawings
Fig. 1 is the preferred embodiment structure diagram of inventive sampling device.
Fig. 2 is the preferred embodiment structure diagram of measuring device of the present invention.
Wherein, reference numeral is:The spherical vacuum target chambers of 1-, 2- target practice laser, 3- target spots, 4- ellipsoid diffusing reflection blanks, 5- sampling windows, 6- sampling diaphragms, 7- imaging lens, 8- veiling glare filters, 9- shrink beam positive lens, 10- dichroscopes, 11- long wave camera sampling mirrors, 12- long wave time measurement sampling mirrors, 13- long wave time measurement coupling mirrors, 14- long waves sampling diaphragm Image planes, 15- long wave spectrums sampling optical fiber, the fast photoelectric tube of 16- long wave time measurements, 17- long wave light absorbs traps, 18- shortwave phases Machine sampling mirror, 19- shortwave time measurement sampling mirrors, 20- shortwave time measurement coupling mirrors, 21- shortwaves sampling diaphragm image planes, 22- Shortwave spectrum samples optical fiber, the fast photoelectric tube of 23- shortwave time measurements, 24- short wavelength lights absorption trap.
Embodiment
The present embodiment is a kind of nearly back-scattering light time measurement system based on ellipsoid diffusing reflection blank, its structure bag Include sampler and measuring device.
Referring to Fig. 1, sampler includes spherical vacuum target chamber 1 and sampling diaphragm 6, and target is provided with spherical vacuum target chamber 1 Point 3 and ellipsoid diffusing reflection blank 4;The nearly back-scattering light that the incident target spot 3 of target practice laser 2 produces along after target practice backscattering by Ellipsoid diffusing reflection blank 4 produces diffusing reflection, is passed through again after diffusing through the sampling window 5 set on spherical vacuum target chamber 1 The sampling sampling of diaphragm 6 enters measuring device;Target spot 3 is located in a focus of ellipsoid diffusing reflection blank 4, sampling diaphragm 6 Center is located in another focus of ellipsoid diffusing reflection blank 4.According to the characteristic of ellipsoid, from target spot 3 to sampling light Each light of door screen 6 is all aplanatic, therefore the sampler realizes no time difference sampling.
Referring to Fig. 2, measuring device includes imaging lens 7, the shrink beam positive lens 9 and two set gradually along paths direction To Look mirror 10;After dichroscope 10 separates spectrum, long wave is transmitted into long wave transmission light measurements unit, shortwave and is reflected into Enter shortwave reflected light measurement unit.
As a kind of preferred embodiment, long wave transmission light measurements unit includes long wave camera sampling mirror 11, the long wave time surveys Measure sampling mirror 12, long wave time measurement coupling mirror 13 and the fast photoelectric tube 16 of long wave time measurement;Long wave transmitted light passes through long wave phase After machine sampling mirror 11, reflected by long wave time measurement sampling mirror 12, length is then imaged in by long wave time measurement coupling mirror 13 again In long wave sampling diaphragm image planes 14 where the fast photoelectric tube 16 of ripple time measurement.In long wave transmission light measurements unit, during long wave Between measurement coupling mirror 13 be incorporated in before imaging lens 7 in light path, 9 three of shrink beam positive lens collectively form one without optical path difference The imaging system of (i.e. without the time difference), sampling diaphragm 6 is imaged in long wave sampling diaphragm image planes 14.Taken from target spot 3 to long wave There is no any optical path difference between each light of sample diaphragm image planes 14, just without poor any time yet.Diaphragm is sampled in long wave Set the fast photoelectric tube 16 of long wave time measurement to be scattered time response measurement at image planes 14, will not be introduced in optical path any Time difference.
Further, long wave light absorbs trap 17 is provided with long wave sampling diaphragm image planes 14, it is not utilized for absorbing The long glistening light of waves.Long wave spectrum sampling optical fiber 15 can also be set in long wave sampling diaphragm image planes 14, for carrying out long scattering of wave light Spectrometry.
As a kind of preferred embodiment, shortwave reflected light measurement unit includes shortwave camera sampling mirror 18, the shortwave time surveys Measure sampling mirror 19, shortwave time measurement coupling mirror 20 and the fast photoelectric tube 23 of shortwave time measurement;Shortwave reflected light passes through shortwave phase After machine sampling mirror 18, reflected, then imaged in again by shortwave time measurement coupling mirror 20 short by shortwave time measurement sampling mirror 19 In shortwave sampling diaphragm image planes 21 where the fast photoelectric tube 23 of ripple time measurement.In shortwave reflected light measurement unit, during shortwave Between measurement coupling mirror 20 be incorporated in before imaging lens 7 in light path, 9 three of shrink beam positive lens collectively form one without optical path difference The imaging system of (i.e. without the time difference), sampling diaphragm 6 is imaged in shortwave sampling diaphragm image planes 21.Taken from target spot 3 to shortwave There is no any optical path difference between each light of sample diaphragm image planes 21, just without poor any time yet.Diaphragm is sampled in shortwave Set the fast photoelectric tube 23 of shortwave time measurement to be scattered time response measurement at image planes 21, will not be introduced in optical path any Time difference.
Further, short wavelength light absorption trap 24 is provided with shortwave sampling diaphragm image planes 21, it is not utilized for absorbing Short wavelength light.In shortwave sampling diaphragm image planes 21 shortwave spectrum can also be set to sample optical fiber 22, for carrying out shortwave scattering light Spectrometry.
It is preferred that imaging lens 7 image in ellipsoid diffusing reflection blank in image planes in the present embodiment, once as Veiling glare filter 8 can be set on face, for filtering out the veiling glare in other directions, ensure that the light beam for entering test device is equal The scattering light produced for ellipsoid diffusing reflection blank.
Nearly back-scattering light time measurement system proposed by the present invention based on ellipsoid diffusing reflection blank can avoid because Scattering surface diffusing reflection introduces the defects of time difference, realizes the scattering time characteristic high-acruracy survey of nearly back-scattering light.

Claims (9)

1. a kind of nearly back-scattering light time measurement system based on ellipsoid diffusing reflection blank, including sampler and measurement fill Put, it is characterised in that:The sampler includes spherical vacuum target chamber and sampling diaphragm, is provided with the spherical vacuum target chamber Target spot and ellipsoid diffusing reflection blank;Target practice laser light incident target spot produce nearly back-scattering light along target practice opposite direction scatter after by Ellipsoid diffusing reflection blank produces diffusing reflection, enters measuring device after the sampled diaphragm sampling that diffuses;The target spot is located at In one focus of ellipsoid diffusing reflection blank, the sampling diaphragm center is located at another focus of ellipsoid diffusing reflection blank On.
2. the nearly back-scattering light time measurement system according to claim 1 based on ellipsoid diffusing reflection blank, it is special Sign is:The measuring device includes imaging lens, shrink beam positive lens and the dichroscope set gradually along paths direction; After the dichroscope separates spectrum, long wave is transmitted into long wave transmission light measurements unit, shortwave and is reflected into shortwave Reflected light measurement unit.
3. the nearly back-scattering light time measurement system according to claim 2 based on ellipsoid diffusing reflection blank, it is special Sign is:The long wave transmission light measurements unit includes long wave time measurement coupling mirror and the fast photoelectric tube of long wave time measurement;It is long Ripple transmitted light samples diaphragm image planes as the long wave where long wave time measurement coupling mirror images in the fast photoelectric tube of long wave time measurement On.
4. the nearly back-scattering light time measurement system according to claim 3 based on ellipsoid diffusing reflection blank, it is special Sign is:Long wave light absorbs trap is provided with the long wave sampling diaphragm image planes.
5. the nearly back-scattering light time measurement system according to claim 4 based on ellipsoid diffusing reflection blank, it is special Sign is:Long wave spectrum sampling optical fiber is additionally provided with the long wave sampling diaphragm image planes.
6. the nearly back-scattering light time measurement system according to claim 2 based on ellipsoid diffusing reflection blank, it is special Sign is:The shortwave reflected light measurement unit includes shortwave time measurement coupling mirror and the fast photoelectric tube of shortwave time measurement;It is short Wave reflection light samples diaphragm image planes as the shortwave where shortwave time measurement coupling mirror images in the fast photoelectric tube of shortwave time measurement On.
7. the nearly back-scattering light time measurement system according to claim 6 based on ellipsoid diffusing reflection blank, it is special Sign is:Short wavelength light absorption trap is provided with the shortwave sampling diaphragm image planes.
8. the nearly back-scattering light time measurement system according to claim 7 based on ellipsoid diffusing reflection blank, it is special Sign is:Shortwave spectrum sampling optical fiber is additionally provided with the shortwave sampling diaphragm image planes.
9. according to any nearly back-scattering light time measurement system based on ellipsoid diffusing reflection blank in claim 2-8 System, it is characterised in that:The imaging lens image in ellipsoid diffusing reflection blank in image planes, are set in an image planes It is equipped with veiling glare filter.
CN201711341523.2A 2017-12-14 2017-12-14 Near back scattered light time measurement system based on ellipsoidal diffuse reflection whiteboard Active CN107966277B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201711341523.2A CN107966277B (en) 2017-12-14 2017-12-14 Near back scattered light time measurement system based on ellipsoidal diffuse reflection whiteboard

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201711341523.2A CN107966277B (en) 2017-12-14 2017-12-14 Near back scattered light time measurement system based on ellipsoidal diffuse reflection whiteboard

Publications (2)

Publication Number Publication Date
CN107966277A true CN107966277A (en) 2018-04-27
CN107966277B CN107966277B (en) 2023-12-08

Family

ID=61995365

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201711341523.2A Active CN107966277B (en) 2017-12-14 2017-12-14 Near back scattered light time measurement system based on ellipsoidal diffuse reflection whiteboard

Country Status (1)

Country Link
CN (1) CN107966277B (en)

Citations (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4156571A (en) * 1977-09-07 1979-05-29 The Singer Company Laser mirror scatter and reflectivity measuring system
GB8908422D0 (en) * 1988-05-09 1989-06-01 Spectra Tech Inc Diffuse reflectance spectroscopy system and method
JP2001281097A (en) * 2000-03-28 2001-10-10 Nikon Corp Method and apparatus for measuring scattered light
WO2003085385A1 (en) * 2002-04-04 2003-10-16 Lla Instruments Gmbh Method and spectrometer for spectrometrically measuring the extinction, transmission, diffuse reflection or the reflection of samples
US20070222984A1 (en) * 2006-03-23 2007-09-27 Palumbo Perry A Optical Design of a Measurement System Having Mulitiple Sensor or Multiple Light Source Paths
WO2009135376A1 (en) * 2008-05-09 2009-11-12 清华大学 Method and device for inspecting object with a forward direction scatter radiation
CN103268009A (en) * 2013-06-07 2013-08-28 北京师范大学 Vertical illumination dark-field microscope
CN105469837A (en) * 2015-12-29 2016-04-06 中国科学院西安光学精密机械研究所 Laser fusion backscattered light beam analog device
CN105489262A (en) * 2015-12-29 2016-04-13 中国科学院西安光学精密机械研究所 Universal point light source simulation system
CN207636277U (en) * 2017-12-14 2018-07-20 中国科学院西安光学精密机械研究所 Nearly back-scattering light time measurement system based on ellipsoid diffusing reflection blank

Patent Citations (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4156571A (en) * 1977-09-07 1979-05-29 The Singer Company Laser mirror scatter and reflectivity measuring system
GB8908422D0 (en) * 1988-05-09 1989-06-01 Spectra Tech Inc Diffuse reflectance spectroscopy system and method
JP2001281097A (en) * 2000-03-28 2001-10-10 Nikon Corp Method and apparatus for measuring scattered light
WO2003085385A1 (en) * 2002-04-04 2003-10-16 Lla Instruments Gmbh Method and spectrometer for spectrometrically measuring the extinction, transmission, diffuse reflection or the reflection of samples
US20070222984A1 (en) * 2006-03-23 2007-09-27 Palumbo Perry A Optical Design of a Measurement System Having Mulitiple Sensor or Multiple Light Source Paths
WO2009135376A1 (en) * 2008-05-09 2009-11-12 清华大学 Method and device for inspecting object with a forward direction scatter radiation
CN103268009A (en) * 2013-06-07 2013-08-28 北京师范大学 Vertical illumination dark-field microscope
CN105469837A (en) * 2015-12-29 2016-04-06 中国科学院西安光学精密机械研究所 Laser fusion backscattered light beam analog device
CN105489262A (en) * 2015-12-29 2016-04-13 中国科学院西安光学精密机械研究所 Universal point light source simulation system
CN207636277U (en) * 2017-12-14 2018-07-20 中国科学院西安光学精密机械研究所 Nearly back-scattering light time measurement system based on ellipsoid diffusing reflection blank

Non-Patent Citations (4)

* Cited by examiner, † Cited by third party
Title
LUO GEN等: "Backscattering from small-scale breaking wave turbulence structure generated by FLUENT", 《CHINESE PHYSICS B》, vol. 23, no. 12, XP020274720, DOI: 10.1088/1674-1056/23/12/124101 *
王峰;彭晓世;杨冬;李志超;徐涛;魏惠月;刘慎业;: "基于神光Ⅲ原型的背向散射实验技术研究", 物理学报, no. 17 *
王峰;彭晓世;闫亚东;徐涛;魏惠月;理玉龙;李楠;: "基于神光III主机的背向散射光诊断技术", 中国激光, no. 09 *
韩洋;何俊华;闫亚东;吴冰静;: "近背向散射测量系统中漫反射板的特性研究", 红外与激光工程, no. 09 *

Also Published As

Publication number Publication date
CN107966277B (en) 2023-12-08

Similar Documents

Publication Publication Date Title
CN102749184B (en) Large field-of-view stray light PST (point source transmittance) testing method and device
CN103197499B (en) A kind of electrophotographic system of framing, scanning ultra high-speed optical simultaneously
Faccio et al. A trillion frames per second: the techniques and applications of light-in-flight photography
CN102564611B (en) High-power laser wave front measuring instrument and wave front measuring method
JPS6026962B2 (en) laser ceilometer
CN111060289B (en) High-sensitivity coronagraph stray light detection device
CN104483676A (en) 3D/2D (Three Dimensional/Two Dimensional) scannerless laser radar compound imaging device
CN202710290U (en) Large visual field stray light PST testing device
KR20130084863A (en) Apparatus for measuring the degree of transmission
CN108693088B (en) Atmospheric particulate monitoring scanning polarization laser radar system
CN104197865B (en) Implementation method of laser auto-collimator with laser beam guide function
CN102539254B (en) Digital laser dynamic caustics experiment method and system thereof
CN207636277U (en) Nearly back-scattering light time measurement system based on ellipsoid diffusing reflection blank
CN106018346A (en) Aerosol scattering phase function observing device and method
CN112213737A (en) Long-distance photon counting three-dimensional laser radar imaging system and method thereof
CN110018494A (en) A kind of system and method promoting muddy underwater laser images resolution ratio
CN104458697A (en) Portable raman spectrum explosive identifier
CN214096364U (en) Raman probe based on double compound eye lens set
CN207636278U (en) The nearly backscattering light measurement system of anti-interference of stray light
CN207636486U (en) Nearly backscattering optics measuring system
CN107966277A (en) Nearly back-scattering light time measurement system based on ellipsoid diffusing reflection blank
CN107991064A (en) The nearly backscattering light measurement system of anti-interference of stray light
CN106645082A (en) Gating optical fiber Raman spectrometer based on laser ranging automatic focusing
CN108333147B (en) Near back scattering optical measurement system
CN206164747U (en) Measurement device for X ray framing camera exposure time

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