CN211954621U - High-precision multi-optical-axis consistency measuring system - Google Patents
High-precision multi-optical-axis consistency measuring system Download PDFInfo
- Publication number
- CN211954621U CN211954621U CN202020626892.7U CN202020626892U CN211954621U CN 211954621 U CN211954621 U CN 211954621U CN 202020626892 U CN202020626892 U CN 202020626892U CN 211954621 U CN211954621 U CN 211954621U
- Authority
- CN
- China
- Prior art keywords
- mirror
- optical axis
- focus
- guide rail
- light source
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Active
Links
Images
Landscapes
- Investigating Or Analysing Materials By Optical Means (AREA)
Abstract
The utility model relates to a many optical axis uniformity are measured, concretely relates to many optical axis uniformity measurement system of high accuracy. The utility model aims at solving the technical problem that the many optical axis uniformity of current many optical axis uniformity measurement system exist can't establish the high accuracy measurement benchmark, be difficult to compromise laser emission optical axis, laser reception optical axis, visible light optical axis, infrared optical axis and measure, provide a many optical axis uniformity measurement system of high accuracy. The system comprises a collimator tube component, a focus component, a sampling mirror component and a long-focus auto-collimation light tube component; the collimator assembly comprises an off-axis parabolic mirror and a folding-axis mirror; the sampling mirror assembly comprises a first sampling mirror and a second sampling mirror, and the second sampling mirror is a semi-transparent semi-reflecting mirror; the long-focus auto-collimation light tube component comprises a convergent lens, a spectroscope, a CCD detector, a second cross target and an area array light source.
Description
Technical Field
The utility model relates to a many optical axis uniformity are measured, concretely relates to many optical axis uniformity measurement system of high accuracy.
Background
With the continuous development of the technology of the airborne photoelectric pod, the photoelectric load is cooperated with other equipment to form the airborne pod to realize the activities such as ground observation and search, and the activities become the main mode of aviation observation and search gradually. In order to further improve the detection capability at night or under low illumination, the photoelectric load system has been developed towards the direction of integrating multi-spectral band detection of visible light, near infrared, medium wave infrared and the like.
Most of the existing airborne pod photoelectric load systems are provided with a plurality of photoelectric detectors such as a visible light distance meter, an infrared distance meter and a laser distance meter. The calibration and measurement of the consistency (i.e. parallelism) between the optical axes of the photoelectric detectors are important links for adjusting and detecting the photoelectric load equipment of the nacelle. Calibrating and measuring the optical axis consistency between multi-spectral band optical axis photodetectors requires establishing a measurement reference that can be simultaneously responded by these photodetectors. Therefore, establishing a high-precision multi-spectral optical axis measurement reference and performing high-precision consistency measurement between multi-spectral optical axes are key points for improving the photoelectric load detection performance of the nacelle.
At present, common methods for measuring the multi-spectral optical axis consistency include common-aperture coaxial clamp type, common-aperture off-axis parabolic type, laser photographic paper detection method and thermal effect target measurement method, and the common defect of the common methods is low measurement reference precision. In addition, although the coaxial card type with the same aperture has the advantage of small volume of a measurement system, the coaxial card type with the same aperture has the defect of central blocking; in the common-aperture off-axis parabolic measurement system, light converged by an off-axis parabolic mirror is transmitted by a semi-transparent and semi-reflective folding axis mirror and then is received by a CCD detector, so that the measurement system is inconvenient for measuring a high-power laser emission optical axis and a laser receiving optical axis, and the measurement precision is low; the laser photographic paper detection method can realize consistency measurement of a laser emission optical axis, a laser receiving optical axis and a visible light optical axis, but the photographic paper exposed by laser irradiation needs to be replaced, so real-time detection cannot be carried out; although the thermal effect target measurement method can realize the consistency measurement of the laser optical axis and the infrared optical axis by converting the emitted laser into infrared radiation, the consistency measurement of the laser optical axis and the visible light optical axis cannot be realized, and the judgment of the consistency deviation needs to utilize an optical axis reference device of a consistency measurement system.
Disclosure of Invention
The utility model aims at solving the technical problem that the many optical axis uniformity of current many optical axis uniformity measurement system exist can't establish the high accuracy measurement benchmark, be difficult to compromise laser emission optical axis, laser reception optical axis, visible light optical axis, infrared optical axis and measure, provide a many optical axis uniformity measurement system of high accuracy.
In order to solve the technical problem, the utility model provides a technical solution as follows:
the utility model provides a many optical axes of high accuracy uniformity measurement system, its special character lies in: the device comprises a collimator tube component, a focus component, a sampling mirror component and a long-focus auto-collimation light tube component;
the collimator assembly comprises an off-axis parabolic mirror and an off-axis mirror, and the off-axis mirror is positioned at the focal plane of the off-axis parabolic mirror;
the focus assembly comprises a target switching guide rail, a light source switching guide rail, a first cross target, ground glass and a simulation laser which are arranged on the target switching guide rail, an integrating sphere and a black body light source, wherein the integrating sphere is arranged on the light source switching guide rail and used for providing visible light, and the black body light source is used for providing infrared radiation;
the target switching guide rail passes through the focus of the collimator tube component, so that the first cross target, the ground glass and the simulation laser can be respectively positioned at the focus of the collimator tube component by moving on the target switching guide rail;
the light source switching guide rail is positioned on one side of the focus of the collimator tube component, so that the integrating sphere blackbody light source can respectively provide visible light and infrared radiation to the focus of the collimator tube component by moving on the light source switching guide rail;
the sampling mirror assembly comprises a first sampling mirror and a second sampling mirror which are arranged vertically, and the second sampling mirror is a semi-transparent semi-reflecting mirror;
the long-focus auto-collimation light tube component comprises a convergent lens, a spectroscope, a CCD detector, a second cross target and an area array light source for illuminating the second cross target;
the first sampling mirror, the second sampling mirror, the convergent lens and the spectroscope are sequentially arranged on a collimation emergent light path of the off-axis parabolic mirror;
the converging lens forms two conjugate focal planes under the action of the spectroscope, the CCD detector is positioned at one focal plane of the converging lens, and the second cross target is positioned at the other focal plane of the converging lens.
Furthermore, the focal length of the off-axis parabolic mirror is 3000mm, and the effective clear aperture is
Furthermore, the convergent lens is of a transmission structure, the focal length is 1000mm, and the effective light-passing aperture is
Further, the pixel size of the CCD detector is 4.8 μm.
Compared with the prior art, the utility model has the following beneficial effects:
1. the utility model provides a many optical axes of high accuracy uniformity measurement system, through the switching of first cross target, ground glass, three targets of simulation laser instrument in collimator subassembly focus department, utilize the integrating sphere to provide visible light, the black body light source provides infrared radiation, the collimator subassembly that adopts the heavy-calibre long focus that off-axis parabolic mirror and jack lens are constituteed converges, the collimation, the sample mirror subassembly sample, combine convergent lens, the spectroscope, the CCD detector, the twentieth target, be used for illuminating the long burnt auto-collimation light pipe subassembly that the area array light source of the twentieth target constitutes receives light and record facula barycenter coordinate, make the optical axis at each target of collimator subassembly focus have the uniformity, and collimator subassembly optical axis and long burnt auto-collimation light pipe subassembly optical axis have the basis of uniformity, establish a many optical axes of high accuracy uniformity measurement benchmark, the high-precision measurement of consistency of multiple optical axes (including visible light optical axes, laser emission optical axes, laser receiving optical axes and infrared optical axes) of the measured photoelectric load is realized, important technical means for adjustment and measurement are provided for guaranteeing the consistency of the multiple optical axes of the airborne photoelectric load, and the high-precision measurement method has great scientific research significance and engineering practical value.
2. The utility model provides a many optical axes of high accuracy uniformity measurement system, when measuring the uniformity of laser emission optical axis and laser receiving optical axis, utilize the method of ground glass scattering sample, ground glass has the effect of decay and scattering, not only solved the problem that high power pulse laser harmd the CCD detector easily ingeniously, and with the visible light optical axis, laser emission optical axis and laser receiving optical axis are introduced into the long burnt auto-collimation fluorescent tube subassembly that is used for image acquisition and processing, compromise laser emission optical axis, laser receiving optical axis, the visible light optical axis, the many optical axes uniformity measuring basis of infrared optical axis has been established.
3. The utility model provides a many optical axes of high accuracy uniformity measurement system, the focus of off-axis parabolic mirror is 3000mm, and effective logical light bore does
The convergent lens is of a transmission structure, the focal length is 1000mm, and the effective light-passing aperture is
The pixel size of the CCD detector is 4.8 mu m, so that the measurement accuracy of the measurement system is better than 2 ', the consistency deviation of the optical axes of all targets of the focal points of the collimator assembly is ensured to be within 5', the consistency deviation of the optical axes of the collimator assembly and the optical axis of the long-focus self-collimating tube assembly is ensured to be within 5 ', the multi-optical-axis consistency measurement reference accuracy is high, meanwhile, the consistency debugging and measurement results of the visible light, infrared radiation and laser emission optical axes and the laser receiving optical axis are enabled to be within 5', and the high-precision assembling and consistency deviation measurement among the photoelectric load multiple optical axes is realized.
Drawings
Fig. 1 is a schematic structural view of the high-precision multi-optic-axis consistency measuring system of the present invention;
FIG. 2 is a schematic view of the collimator assembly of the high-precision multi-optic-axis consistency measuring system of the present invention for converging and collimating light;
fig. 3 is a schematic diagram of the converging lens of the high-precision multi-optic-axis consistency measuring system of the present invention, wherein two lenses on the right represent the converging lens, and the focal plane of the converging lens is on the left;
description of reference numerals:
1-a collimator assembly; 101-off-axis parabolic mirror; 102-a folding axis mirror;
2-a focal assembly; 201-target switching guide rail; 2011-first cross target; 2012-ground glass; 2013-analog laser; 202-light source switching guide; 2021-integrating sphere; 2022-blackbody light source;
3-a sampler mirror assembly; 301-a first sampling mirror; 302-a second sampling mirror;
4-a long-focus auto-collimation light pipe component; 401-a convergence lens; 402-a beam splitter; 403-a CCD detector; 404-second cross target; 405-area array light source;
5-measured photoelectric load.
Detailed Description
The present invention will be further described with reference to the accompanying drawings.
The utility model provides a high-precision multi-optical-axis consistency measuring system, as shown in figure 1, comprising a collimator tube component 1, a focus component 2, a sampling mirror component 3 and a long-focus auto-collimation tube component 4; the collimator assembly 1 comprises an off-axis parabolic mirror 101 and an off-axis mirror 102, wherein the off-axis mirror 102 is positioned at the focal plane of the off-axis parabolic mirror 101; the focus assembly 2 comprises a target switching guide rail 201, a light source switching guide rail 202, a first cross target 2011, ground glass 2012 and a simulated laser 2013 which are arranged on the target switching guide rail 201, and an integrating sphere 2021 and a black body light source 2022 which are arranged on the light source switching guide rail 202 and are used for providing visible light and infrared radiation; the target switching guide rail 201 passes through the focus of the collimator tube assembly 1, so that the first cross target 2011, the ground glass 2012 and the simulated laser 2013 are respectively positioned at the focus of the collimator tube assembly 1 by moving on the target switching guide rail 201; the light source switching guide rail 202 is positioned on one side of the focus of the collimator assembly 1, so that the integrating sphere 2021 and the blackbody light source 2022 can respectively provide visible light and infrared radiation to the focus of the collimator assembly 1 by moving on the light source switching guide rail 202; the sampling mirror assembly 3 comprises a first sampling mirror 301 and a second sampling mirror 302 which are arranged vertically to each other, and the second sampling mirror 302 is a half-transmitting and half-reflecting mirror; the long-focus autocollimation light pipe component 4 comprises a convergent lens 401, a spectroscope 402, a CCD detector 403, a second cross target 404 and an area array light source 405 for illuminating the second cross target 404; the first sampling mirror 301, the second sampling mirror 302, the convergent lens 401 and the spectroscope 402 are sequentially arranged on a collimation emergent light path of the off-axis parabolic mirror 101; the converging lens 401 forms two conjugate focal planes under the action of the beam splitter 402, the CCD detector 403 is located at one focal plane of the converging lens 401, and the second cross target 404 is located at the other focal plane of the converging lens 401.
The focal length of the off-axis parabolic mirror 101 is 3000mm, and the effective clear aperture is
The convergent lens 401 is a transmission structure, the focal length is 1000mm, and the effective light-passing aperture is
The pixel size of the CCD detector 403 is 4.8 μm.
The method for measuring the consistency of the multi-optical axis with high precision by using the system comprises the following steps:
1) multi-optical axis consistency measurement benchmarking
1.1) consistency calibration and debugging of optical axes of targets at focus of collimator assembly 1
1.1.1) moving a first cross target 2011 to a focus of a collimator assembly 1 by using a target switching guide rail 201 to serve as a target, moving an integrating sphere 2021 by using a light source switching guide rail 202 to enable uniform visible light emitted by the integrating sphere 2021 to illuminate a target surface of the first cross target 2011, emitting cross visible light from the first cross target 2011, collimating the first cross visible light by the collimator assembly 1 and then emitting the cross visible light in parallel, reflecting a part of the parallel emitted light by a sampling mirror assembly 3, transmitting the part of the parallel emitted light by a converging lens 401, and splitting the part of the parallel emitted light by a beam splitter 402 to reach a focus surface of a CCD detector 403 to obtain a first cross target image, and extracting the first cross target image by the CCD detector 403 through a software algorithm to mark the first cross target image as;
1.1.2) replacing the first cross target 2011 with ground glass 2012 and replacing the integrating sphere 2021 with a black body light source 2022, repeating the operation of the same procedure as the step 1.1), obtaining the center of mass coordinate of the ground glass 2012, and finely adjusting the posture of the ground glass 2012 to enable the deviation between the center of mass coordinate of the ground glass 2012 and the origin coordinate obtained in the step 1.1) to be within 5';
1.1.3) replacing the first cross target 2011 with a simulated laser 2013, removing an integrating sphere 2021, repeating the operation of the same program as the step 1.1), obtaining the centroid coordinate of the simulated laser, finely adjusting the posture of the simulated laser 2013, and enabling the centroid coordinate of the simulated laser and the origin coordinate obtained in the step 1.1) to be within 5 ″, wherein at the moment, the consistency calibration and the debugging of the optical axis of each target at the focus of the collimator assembly 1 are completed;
1.2) debugging the consistency of the optical axis of the collimator assembly 1 and the optical axis of the long-focus auto-collimation light pipe assembly 4
1.2.1) placing an octahedron combination pyramid which plays a plane reflection role in the horizontal direction of the second sampling mirror 302, illuminating a second cross target 404 by using an area array light source 405, emitting cross visible light from the second cross target 404, emitting the cross visible light in parallel through a convergent lens 401, reflecting the cross visible light by the octahedron combination pyramid, returning the cross visible light to the original path, receiving a reflected second cross target image by a focal plane of a CCD detector 403, extracting the centroid of the reflected second cross target image, and marking the centroid as the centroid coordinate of the second cross target 404;
1.2.2) turning off the area array light source 405, turning on an integrating sphere 2021 to illuminate the first cross target 2011, collimating the cross visible light emitted from the first cross target 2011 by the collimator tube component 1, reflecting the cross visible light by the sampling mirror component 3, and then reaching the focal plane of the CCD detector 403 to extract the centroid of the cross visible light, wherein the centroid is marked as the centroid coordinate of the first cross target 2011;
1.2.3) adjusting the posture of the sampling mirror assembly 3 to ensure that the centroid coordinate deviation of the first cross target 2011 and the second cross target 404 is within 5 ″, because the optical axis of the first cross target 2011 represents the optical axis of the collimator tube assembly 1 and the optical axis of the second cross target 404 represents the optical axis of the long-focus auto-collimation tube assembly 4, the optical axis of the collimator tube assembly 1 is consistent with the optical axis of the long-focus auto-collimation tube assembly 4, and the multi-optical-axis consistency measurement reference is established;
2) measured optoelectric load 5 multi-optic axis consistency measurement
2.1) measured photoelectric load 5 attitude adjustment
Adjusting the pitching and azimuth postures of the measured photoelectric load 5 to enable the installation reference axis of the measured photoelectric load 5 to be parallel to the high-precision multi-optical-axis consistency measurement system;
2.2) laser emission optical axis coordinate measurement
Switching the ground glass 2012 to the focus of the collimator tube component 1, emitting high-power pulse laser by the measured photoelectric load 5, converging the high-power pulse laser on the ground glass 2012 through the collimator tube component 1, attenuating and scattering incident laser by the ground glass 2012, collimating the scattered laser through the collimator tube component 1, reflecting by the sampling mirror component 3, transmitting through the converging lens 401, and splitting by the beam splitter 402, and then reaching the focal plane of the CCD detector 403, extracting the centroid of the laser spot, and marking the laser spot as the laser emission optical axis coordinate;
2.3) laser receiver optical axis coordinate measurement
Switching the simulated laser 2013 to the focus of the collimator tube component 1, enabling the simulated laser 2013 to emit simulated laser, collimating the simulated laser by the collimator tube component 1, emitting the simulated laser in parallel, receiving the collimated laser by a detector carried by a laser receiving device of the tested photoelectric load 5, and performing mass center extraction on the simulated laser by the detector to mark the simulated laser as a laser receiving optical axis coordinate;
2.4) measurement of the coordinates of the visible light axis
The first cross target 2011 is switched to the focus of the collimator assembly 1, the integrating sphere 2021 is aligned to the first cross target 2011 through the light source switching guide rail 202, the uniform visible light emitted by the integrating sphere 2021 illuminates the first cross target 2011, the first cross target 2011 emits cross visible light, the cross visible light is collimated by the collimator assembly 1 and then emitted in parallel, and the collimated light is received by the visible light system of the measured photoelectric load 5, and the visible light system extracts the centroid of the cross visible light and marks the centroid as the optical axis coordinate of the visible light;
2.5) Infrared optical axis coordinate measurement
The blackbody light source 2022 is aligned to the first cross target 2011 through the light source switching guide rail 202, the infrared radiation emitted by the blackbody light source 2022 illuminates the first cross target 2011, the first cross target 2011 emits cross infrared radiation, the cross infrared radiation is collimated by the collimator tube assembly 1 and then emitted in parallel, the collimated infrared radiation is received by the infrared system of the measured photoelectric load 5, the infrared system performs centroid extraction on the cross infrared radiation, and the centroid extraction is marked as an infrared optical axis coordinate;
2.6) calculating consistency deviation values among the optical axes of the tested photoelectric load 5 by utilizing the laser emission optical axis coordinate, the laser receiving optical axis coordinate, the visible light optical axis coordinate and the infrared optical axis coordinate which are respectively obtained in the steps 2.2) to 2.5), and correspondingly adjusting the optical axes of the tested photoelectric load 5 according to the deviation values to enable the consistency deviation among the laser emission optical axis, the laser receiving optical axis, the visible light optical axis and the infrared optical axis to be within 5 ″, wherein the high-precision measurement of the multi-optical-axis consistency of the tested photoelectric load 5 is completed.
FIG. 2 is a schematic view of the collimator assembly 1 of the high-precision multi-optic-axis consistency measuring system according to the present invention for converging and collimating light; fig. 3 is the utility model discloses high accuracy multiaxis uniformity measurement system's convergent lens convergent light line sketch map, two lenses on the right side represent convergent lens, and the left side is convergent lens's focal plane.
Finally, it should be noted that: the above embodiments are only used for illustrating the technical solutions of the present invention, and not for limiting the same, and it is obvious for a person skilled in the art to modify the specific technical solutions described in the foregoing embodiments or to equally replace some technical features of the embodiments, and these modifications or replacements do not make the essence of the corresponding technical solutions depart from the scope of the technical solutions protected by the present invention.
Claims (4)
1. The utility model provides a many optical axes of high accuracy uniformity measurement system which characterized in that: comprises a collimator tube component (1), a focus component (2), a sampling mirror component (3) and a long-focus auto-collimation light tube component (4);
the collimator tube assembly (1) comprises an off-axis parabolic mirror (101) and a folding axis mirror (102), wherein the folding axis mirror (102) is positioned at the focal plane of the off-axis parabolic mirror (101);
the focus assembly (2) comprises a target switching guide rail (201), a light source switching guide rail (202), a first cross target (2011), ground glass (2012) and a simulated laser (2013) which are arranged on the target switching guide rail (201), an integrating sphere (2021) which is arranged on the light source switching guide rail (202) and used for providing visible light, and a black body light source (2022) which is used for providing infrared radiation;
the target switching guide rail (201) passes through the focus of the collimator tube component (1), so that the first cross target (2011), the ground glass (2012) and the simulation laser (2013) can be respectively positioned at the focus of the collimator tube component (1) by moving on the target switching guide rail (201);
the light source switching guide rail (202) is positioned on one side of the focus of the collimator tube component (1), so that the integrating sphere (2021) and the blackbody light source (2022) can respectively provide visible light and infrared radiation to the focus of the collimator tube component (1) by moving on the light source switching guide rail (202);
the sampling mirror assembly (3) comprises a first sampling mirror (301) and a second sampling mirror (302) which are arranged vertically to each other, and the second sampling mirror (302) is a half-transmitting half-reflecting mirror;
the long-focus auto-collimation light pipe assembly (4) comprises a convergent lens (401), a spectroscope (402), a CCD detector (403), a second cross target (404) and an area array light source (405) for illuminating the second cross target (404);
the first sampling mirror (301), the second sampling mirror (302), the convergent lens (401) and the spectroscope (402) are sequentially arranged on a collimation emergent light path of the off-axis parabolic mirror (101);
the converging lens (401) forms two conjugate focal planes under the action of the spectroscope (402), the CCD detector (403) is positioned at one focal plane of the converging lens (401), and the second cross target (404) is positioned at the other focal plane of the converging lens (401).
2. The high accuracy multi-optic axis consistency measurement system of claim 1, wherein: the focal length of the off-axis parabolic mirror (101) is 3000mm, and the effective clear aperture is
。
3. The high accuracy multi-optic axis consistency measurement system of claim 2, wherein: the convergent lens (401) is of a transmission structure, the focal length is 1000mm, and the effective light-passing aperture is
。
4. A high accuracy multi-optic axis consistency measurement system according to claim 1, 2 or 3, characterized by: the pixel size of the CCD detector (403) is 4.8 mu m.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN202020626892.7U CN211954621U (en) | 2020-04-23 | 2020-04-23 | High-precision multi-optical-axis consistency measuring system |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN202020626892.7U CN211954621U (en) | 2020-04-23 | 2020-04-23 | High-precision multi-optical-axis consistency measuring system |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CN211954621U true CN211954621U (en) | 2020-11-17 |
Family
ID=73161954
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN202020626892.7U Active CN211954621U (en) | 2020-04-23 | 2020-04-23 | High-precision multi-optical-axis consistency measuring system |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN211954621U (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN111442910A (en) * | 2020-04-23 | 2020-07-24 | 中国科学院西安光学精密机械研究所 | High-precision multi-optical-axis consistency measurement system and method |
-
2020
- 2020-04-23 CN CN202020626892.7U patent/CN211954621U/en active Active
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN111442910A (en) * | 2020-04-23 | 2020-07-24 | 中国科学院西安光学精密机械研究所 | High-precision multi-optical-axis consistency measurement system and method |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CN111442910A (en) | High-precision multi-optical-axis consistency measurement system and method | |
| CN110186653B (en) | Optical axis consistency calibration and split image fixed focus adjustment device and method for non-imaging system | |
| US7064817B1 (en) | Method to determine and adjust the alignment of the transmitter and receiver fields of view of a LIDAR system | |
| CN108050933B (en) | Pyramid prism retroreflection light spot positioning precision detection device and method | |
| CN103884491B (en) | A kind of scanning camera pendulum mirror two dimension dynamic angular measures calibration steps and device | |
| CN105044704B (en) | The spaceborne laser transmitter integrated test system for performance of high accuracy | |
| CN208520336U (en) | Laser datum bridge Multi-point deflection vision inspection apparatus | |
| CN109373816A (en) | A kind of laser facula and echo tracking monitoring device | |
| CN101476844B (en) | Calibration method and standard target plate for carrier optoelectronic series on-site dynamic self-calibration | |
| CN109580177B (en) | Airborne three-optical axis consistency testing assembly, system and testing method | |
| Niu et al. | Design of a new multispectral waveform LiDAR instrument to monitor vegetation | |
| CN110146259A (en) | A kind of reflective multi-light axis consistency quantitative test of large-caliber off-axis and calibrating installation | |
| CN101726358B (en) | Co-graduation surface full-spectrum target | |
| CN104483099B (en) | A kind of detection method of large visual field optical system image planes uniformity | |
| CN111707449B (en) | Multi-spectral optical axis parallelism testing device and testing method | |
| CN202522516U (en) | Optical transmissivity test device | |
| CN109870294B (en) | Optical axis parallelism detection device capable of expanding diameter in large range | |
| CN106767545A (en) | A kind of high accuracy high-space resolution angel measuring instrument and angle measurement method | |
| CN104198055A (en) | Wave surface detecting device | |
| CN208239052U (en) | A kind of spuious optical measurement instrument of laser | |
| CN116499709A (en) | High-precision detection device and detection method for pointing error of laser beam | |
| CN211954621U (en) | High-precision multi-optical-axis consistency measuring system | |
| CN209147825U (en) | A kind of laser facula and echo tracking monitoring device | |
| CN106908804A (en) | A kind of forestry plant three-dimensional point cloud measures laser radar system and method | |
| CN105091797B (en) | A kind of single CCD intensity correlation autocollimator |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| GR01 | Patent grant | ||
| GR01 | Patent grant |