CN107765426A - Self-focusing laser scanning projection device based on symmetrical defocus double detector - Google Patents

Self-focusing laser scanning projection device based on symmetrical defocus double detector Download PDF

Info

Publication number
CN107765426A
CN107765426A CN201710992009.9A CN201710992009A CN107765426A CN 107765426 A CN107765426 A CN 107765426A CN 201710992009 A CN201710992009 A CN 201710992009A CN 107765426 A CN107765426 A CN 107765426A
Authority
CN
China
Prior art keywords
focusing
laser
defocus
self
symmetrical
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
CN201710992009.9A
Other languages
Chinese (zh)
Other versions
CN107765426B (en
Inventor
李丽娟
侯茂盛
朱运东
林雪竹
郭丽丽
刘涛
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.)
Shengke Liwei Shenyang Precision Optoelectronic Technology Co ltd
Original Assignee
Changchun University of Science and Technology
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 Changchun University of Science and Technology filed Critical Changchun University of Science and Technology
Publication of CN107765426A publication Critical patent/CN107765426A/en
Application granted granted Critical
Publication of CN107765426B publication Critical patent/CN107765426B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B26/00Optical devices or arrangements for the control of light using movable or deformable optical elements
    • G02B26/08Optical devices or arrangements for the control of light using movable or deformable optical elements for controlling the direction of light
    • G02B26/10Scanning systems
    • G02B26/101Scanning systems with both horizontal and vertical deflecting means, e.g. raster or XY scanners
    • 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
    • G02B27/40Optical focusing aids
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B7/00Mountings, adjusting means, or light-tight connections, for optical elements
    • G02B7/02Mountings, adjusting means, or light-tight connections, for optical elements for lenses
    • G02B7/04Mountings, adjusting means, or light-tight connections, for optical elements for lenses with mechanism for focusing or varying magnification
    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03BAPPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
    • G03B21/00Projectors or projection-type viewers; Accessories therefor
    • G03B21/14Details
    • G03B21/142Adjusting of projection optics

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Length Measuring Devices By Optical Means (AREA)

Abstract

Self-focusing laser scanning projection device based on symmetrical defocus double detector belongs to advanced processing and manufacturing technology.Prior art focuses that the degree of accuracy is low, and the transverse resolution of the automatic search sweep of light intensity is low.Present invention be characterized in that twin shaft scanning galvanometer is set after quarter wave plate;Symmetrical defocus double detector light intensity detection module is set in the demarcation reflected light light path of polarization splitting prism;In symmetrical defocus double detector light intensity detection module, one group of convergence object lens, point detecting pinhole and photodetector are respectively equipped with transmission, reflected light path in Amici prism, for point detecting pinhole between convergence object lens and photodetector, the photosurface of two photodetectors is respectively relative to each self-corresponding convergence object lens defocus+Δ Z, Δ Z;The respective light intensity electrical signal of two photodetectors is connected respectively to two light intensity input end of analog signal of measurement control module;The focusing driving signal output end of measurement control module is connected to the accurate displacement mechanism in dynamic self-focusing module.

Description

Self-focusing laser scanning projection device based on symmetrical defocus double detector
Technical field
The present invention relates to a kind of self-focusing laser scanning projection device based on symmetrical defocus double detector, in intelligence manufacture In assembling process, the laser assisted for various parts is processed (such as composite laying, covering bore riveting, welding) and referred to Show positioning assembling, realize that laser scan round projects by scanning galvanometer, the parts three-dimensional profile that will be driven by three-dimensional CAD digital-to-analogue Profile laser wire frame accurate projection is shown in target processing and assembly area, belongs to advanced processing and manufacturing technology.
Background technology
Laser scanning projection's device be it is a kind of can be by parts to be processed or to be assembled, that is, workpiece to be projected Three-dimensional profile profile by laser beam scan round project in a manner of be converted to laser wire frame and be shown in target processing and dress With region, the region also known as projects and accepts region, so as to realize the accurate photoelectricity of various parts machinings and assembling auxiliary instruction Instrument.
In existing laser scanning projection's device, as shown in figure 1, laser 1, focus module 2, Amici prism 3 are same successively Axle arranges;Twin shaft scanning galvanometer 4 is set in the transmitted light light path of Amici prism 3;In the demarcation reflected light light path of Amici prism 3 Upper setting light intensity detection module 5;The light intensity electrical signal of light intensity detection module 5 is connected to the simulation of measurement control module 6 Signal input part;Computer 7 is connected with measurement control module 6 by USB port;Measure the focusing driving letter of control module 6 Number output end is connected to the accurate displacement mechanism 8 in focus module 2;The scanning drive signal output end for measuring control module 6 connects The precision rotation angle mechanism 9 being connected in twin shaft scanning galvanometer 4.The measurement control module 6 is one piece of multifunctional data acquisition card, energy Enough collections, storage and processing data, the processing include digital-to-analogue, analog-to-digital conversion.
Laser scanning projection's device is the focusing adjustment of scanning projection laser facula first in the course of the work.Swash The scanning projection laser that light device 1 is emitted successively projects to projection by focus module 2, Amici prism 3 and twin shaft scanning galvanometer 4 and held Region 10 is connect, by operating personnel's eye-observation and judges that the focus condition of the laser facula in region 10 is accepted in projection, passes through key Accurate displacement mechanism 8 of the disk operation from measurement control module 6 into focus module 2 sends control signal, drives accurate displacement machine Structure 8 is movable, and until the laser facula observed reaches minimum, it is accurate along focusing for optical axis direction farthest to ensure Degree, complete the focusing adjustment of scanning projection laser facula.
It can be seen that prior art fails to be distributed come automatic feedback control using the light path of the demarcation reflected light of scanning projection laser The focusing adjustment of scanning projection laser facula, the raising for focusing the degree of accuracy are extremely limited.
Next to that calculate the projected coordinate system (P-X of twin shaft scanning galvanometer 4PYPZP) and workpiece three-dimensional CAD digital-to-analogue to be projected Digital-to-analogue coordinate system (O-XOYOZO) between transformational relation.
Because twin shaft scanning galvanometer 4 is precision corner device, it can not learn that the position in region 10 is accepted in projection, can not determine Where reflect the laser wire frame 16 of parts three-dimensional profile contour feature to be projected should be scanned projection.This is just it needs to be determined that throw Shadow accepts the position in region 10, and establishes the D coordinates value of arbitrfary point in workpiece three-dimensional CAD digital-to-analogue to be projected and swept with twin shaft The corresponding relation of the vertical scanning mirror 12 and the scan angle angle value of horizontal scan mirror 13 in galvanometer 4 is retouched, that is, establishes twin shaft scanning Projected coordinate system (the P-X of galvanometer 4PYPZP) with the digital-to-analogue coordinate system (O-X of workpiece three-dimensional CAD digital-to-analogue to be projectedOYOZO) between turn Change relation.
The needs resolved according to equation with many unknowns, the scanning mark that 4 to 6 irregular distributions are chosen in region 10 is accepted in projection Positioning is put, and each scanning calibration position is in digital-to-analogue coordinate system (O-XOYOZO) in three-dimensional coordinate be known.Each swept described Retouch and a back-reflection cooperative target 11 is respectively arranged in calibration position, demarcated for scanning.Swept by what measurement control module 6 was sent Drive signal is retouched by driving two precision rotation angle mechanisms 9 in twin shaft scanning galvanometer 4 to drive respectively in twin shaft scanning galvanometer 4 Vertical scanning mirror 12 and horizontal scan mirror 13, the reflective areas of scanning back-reflection cooperative target 11, one of scanning projection laser Divide and reflected by back-reflection cooperative target 11, returned as demarcation reflected light along original optical path, light intensity is totally reflected to by Amici prism 3 Detecting module 5, converged on photodetector 15 by convergence object lens 14 in light intensity detection module 5, entered by photodetector 15 Row opto-electronic conversion obtains light intensity electric signal, and sends measurement control module 6 to.Control module 6 is measured according to light intensity value of electrical signals And the 13 respective deflection angle of vertical scanning mirror 12 and horizontal scan mirror when obtaining the light intensity electric signal, detect a back of the body To the light intensity peak region of the reflective areas of reflection cooperative target 11, the regional center point is exactly the scanning calibration position, thirdly Dimensional coordinate values are corresponding with a pair of deflection angle angle value, and the high accuracy scanning for completing a center of back-reflection cooperative target 11 is fixed Position.Said process is repeated, the reflective areas of each back-reflection cooperative target 11 is scanned one by one, obtains each group three-dimensional coordinate Value and deflection angle angle value, it thus can accurately calculate the projected coordinate system (P-X of twin shaft scanning galvanometer 4PYPZP) and work to be projected Digital-to-analogue coordinate system (the O-X of part three-dimensional CAD digital-to-analogueOYOZO) between transformational relation.
It can be seen that, if it is possible to strengthen the transverse resolution of the automatic search sweep of light intensity of laser scanning projection's device, it will More accurately calculate the projected coordinate system (P-X of twin shaft scanning galvanometer 4PYPZP) with the digital-to-analogue of workpiece three-dimensional CAD digital-to-analogue to be projected Coordinate system (O-XOYOZO) between transformational relation.
Finally, the three-dimensional profile profile for completing workpiece to be projected accepts the laser scanning projection in region 10 in projection.It will treat Projection workpiece three-dimensional CAD digital-to-analogue is imported into measurement control module 6, position, chi in workpiece three-dimensional CAD digital-to-analogue to be projected The contour feature information such as very little and shape, accurately deflection and the Rapid Circulation scanning of driving twin shaft scanning galvanometer 4, by three-dimensional CAD digital-to-analogue The definition that the contour feature information such as position, size and dimension to workpiece to be projected is done, and according to described two coordinate systems Transformational relation, during the three-dimensional profile profile of workpiece to be projected is circulated including accepting region 10 in projection exactly, form laser Wire frame 16.
It is it can be seen that in actual applications that the parts three-dimensional profile profile laser wire frame driven by three-dimensional CAD digital-to-analogue is accurate Projection Display is processed in target and assembly area, this quality factor for influenceing scanning projection positional accuracy are scanning projection laser Focusing, its influence to scanning projection positional accuracy are presented with following two aspect:
First, the line width for the laser wire frame 16 that laser scanning projection goes out, i.e., be scanned projection in region 10 is accepted in projection When, minimum dimension that laser facula can reach.Scanning projection laser line focus module 2 is in region 10 is accepted in projection along optical axis Direction focuses that the degree of accuracy is higher, the size of laser facula with regard to smaller, the laser wire frame 16 of laser facula scan round projection Line width is narrower, accurately secondary process and instruction can more assemble;
Second, Scan orientation precision of the twin shaft scanning galvanometer 4 to the center of back-reflection cooperative target 11.Work as laser light Spot size is smaller, and transverse resolution of the laser facula in the automatic search sweep of progress light intensity in back-reflection cooperative target 11 is just Stronger, twin shaft scanning galvanometer 4 can just carry out finer scanning with smaller sweep spacing, meanwhile, light intensity detection module 5 The intensity signal of the demarcation reflected lights of more scanning calibration positions can be obtained, also just can more accurately be obtained and back-reflection A pair of deflection angle angle value corresponding to the center of cooperative target 11, and then calculate more accurately coordinate system transformational relation.
The optical maser wavelength that laser 1 in existing laser scanning projection's device is emitted is 532nm, back-reflection cooperation The a diameter of 6mm in reflective areas of target 11, reflectorized material is glass microballoon, and optimal laser scanning projection's orientation distance is 3~5m, 5m apart from when a width of 0.5mm of laser scanning design lines, laser scanning projection's positional accuracy is defined as the half line of laser beam Width, positional accuracy 0.25mm.
The content of the invention
It is it is an object of the present invention to true in the scanning accuracy of twin shaft scanning galvanometer 4 and the control accuracy of measurement control module 6 On the premise of fixed, the focus degree of accuracy of the scanning projection laser of the outgoing of laser 1 along optical axis direction is further improved, obtains size Minimum laser facula, and improve the transverse resolution of the automatic search sweep of light intensity, therefore, we have invented one kind based on pair Claim the self-focusing laser scanning projection device of defocus double detector.Because the positional accuracy of laser scanning projection is with laser half line Width definition, therefore, the raising for focusing the degree of accuracy directly determines the raising of the positional accuracy of laser scanning projection;Due to The transverse resolution of the automatic search sweep of light intensity is directly connected to projected coordinate system (P-XPYPZP) and digital-to-analogue coordinate system (O- XOYOZO) transformational relation resolving accuracy, therefore, the raising of transverse resolution equally also directly determines laser scanning projection Positional accuracy raising.
As shown in Fig. 2 its composition of the self-focusing laser scanning projection device based on symmetrical defocus double detector of the present invention Part includes, and laser 1, twin shaft scanning galvanometer 4, measurement control module 6, computer 7, computer 7 connect with measurement control module 6 Connect;The scanning drive signal output end of measurement control module 6 is connected to the precision rotation angle mechanism 9 in twin shaft scanning galvanometer 4, described It is one piece of multifunctional data acquisition card to measure control module 6;Characterized in that, laser 1, beam-expanding collimation microscope group 17, dynamically from Focus module 18, polarization splitting prism 19, quarter wave plate 20 sequentially coaxially arrange;In the scanning transmission light of polarization splitting prism 19 In light path, and twin shaft scanning galvanometer 4 is set after quarter wave plate 20;In the demarcation reflected light light path of polarization splitting prism 19 Symmetrical defocus double detector light intensity detection module 21 is set;In symmetrical defocus double detector light intensity detection module 21, it is being divided One group of convergence object lens 14, point detecting pinhole 23 and photodetector 15, point detection are respectively equipped with the transmission of prism 22, reflected light path Between convergence object lens 14 and photodetector 15, the photosurface of two photodetectors 15 is respectively relative to each pin hole 23 14 defocus of corresponding convergence object lens+Δ Z ,-Δ Z;The respective light intensity electrical signal of two photodetectors 15 connects respectively To two light intensity input end of analog signal of measurement control module 6;Measure the focusing driving signal output end connection of control module 6 To the accurate displacement mechanism 8 in dynamic self-focusing module 18.
If any one in two photodetectors 15 is located at rear focus, the axial intensity response curve detected For the axial intensity response curve at rear focus, i.e. curve 0 in Fig. 3;Actually two photodetectors 15 separately detect To axial intensity response curve to deviate at rear focus-Δ Z and deviateing the axial intensity response curve at rear focus+Δ Z, That is curve 1 and curve 2 in Fig. 3.From the point of view of now, with zero point O, the light intensity value of curve 1 and curve 2 just corresponds to the light of curve 0 About 0.707 times of intensity values, and the light intensity for demarcating reflected light is maintained at the atomic weak magnitude of tens of micromicrowatts (pW) originally, seems this The effect of invention is run counter to desire, however, on this condition, can by difference and plus and in a manner of be controlled, it is pre- so as to obtain Phase effect.
The light intensity signal of curve 1 and curve 2 is subtracted each other point by point by measurement control module 6, obtains the response of difference axial intensity Curve 3 in curve, i.e. Fig. 3, curve 3 are accurately corresponding in zero point O and the peak point P of curve 0.Slope of the curve 0 near P points connects It is bordering on zero, that is, change of the change to the displacement of accurate displacement mechanism 8 of light intensity value is insensitive, even if controlling mould by measurement Block 6 sends feedback control signal according to curve 0 to dynamic self-focusing module 18, controls accurate displacement mechanism 8 therein to realize and sweeps The axial self-focusing of projection laser hot spot is retouched, rather than eye-observation manual focusing, scanning projection laser focus along optical axis direction The degree of accuracy still is difficult to improve.Although curve 3 is zero in zero point O light intensity, curve 3 zero point O maximum slope, That is change maximum with axial displacement light intensity herein, and it is so far visible, using curve 3 and this particular kind of relationship of curve 0, by surveying Measure control module 6 and send feedback control signal to dynamic self-focusing module 18, control accurate displacement mechanism 8 therein to realize scanning The axial self-focusing of projection laser hot spot, existing eye-observation manual focusing mode, and axial focusing essence can not only be substituted Degree can be improved significantly.
Curve 1 is added point by point with the light intensity signal of curve 2 by measurement control module 6, obtains plus is responded with axial intensity Curve 4 in curve, i.e. Fig. 3;The peak point P " of curve 4 is corresponding with the peak point P of curve 0, and the peak value of curve 4 is about curve 0 1.414 times of peak value, therefore, compared to existing simple detector laser scanning projection apparatus and method, the present invention can be to backwards Reflection cooperative target 11 carry out high-precision transversal scanning positioning, so as to it is sensitiveer, more accurately establish projected coordinate system (P-XPYPZP) and digital-to-analogue coordinate system (O-XOYOZO) between transformational relation.
It can be seen that differential type light intensity detection method is combined by the present invention with plus with formula light intensity detection method, takes into account raising and swash The axial direction of optical scanning projection arrangement focuses ability and transversal scanning resolution capability.
Beam-expanding collimation microscope group 17 is set to improve the numerical aperture 3 to 5 of the focusing microscope group in dynamic self-focusing module 18 Times.According to convergence object lens imaging theory, its spot diameter d is drawn by following formula:
In formula:λ is optical maser wavelength, and nsin α are the numerical aperture of convergence microscope group.It can be seen that the numerical value of increase convergence microscope group Aperture, the theoretical diameter of convergence hot spot can be reduced.When laser wavelength lambda is 532nm, the operating distance for converging microscope group is 4600mm When, convergence microscope group combined focal length is about 2500mm or so, and effective aperture of the laser light incident in convergence microscope group is 12mm, can be calculated The theoretical diameter for obtaining Airy disc is about 0.27mm, it is meant that the theory orientation degree of accuracy brings up to 0.135mm.Limited scanning projects Laser spot size, the subsidiary effect for improving scanning projection laser facula convergence quality is scanning projection laser spot size It is smaller, the size of the reflective areas in the back-reflection cooperative target 11 can be reduced therewith, be such as decreased to 4~5mm, this just anticipates Taste, which, to carry out accurate laser scanning projection in more compact, narrower projection undertaking region 10, and therefore can be expanded Open up the application field of the present invention.
Brief description of the drawings
Fig. 1 is the structural representation of existing laser scanning projection's device.
Fig. 2 is the self-focusing laser scanning projection apparatus structure schematic diagram based on symmetrical defocus double detector of the present invention.
Fig. 3 is the axle obtained using the self-focusing laser scanning projection device based on symmetrical defocus double detector of the present invention To Intensity response curve map, vertical pivot is light intensity I, and transverse axis is axially to normalize coordinate u, in figure:
Curve 0 is the axial intensity response curve that detector is located at rear focus;
Curve 1 is the axial intensity response curve that detector is located off at rear focus-Δ Z;
Curve 2 is the axial intensity response curve that detector is located off at rear focus+Δ Z;
Curve 3 is difference axial intensity response curve;
Curve 4 is to add and axial intensity response curve.
Embodiment
As shown in Fig. 2 its composition of the self-focusing laser scanning projection device based on symmetrical defocus double detector of the present invention Part includes, and laser 1, twin shaft scanning galvanometer 4, measurement control module 6, computer 7, computer 7 connect with measurement control module 6 Connect;The scanning drive signal output end of measurement control module 6 is connected to the precision rotation angle mechanism 9 in twin shaft scanning galvanometer 4, described It is one piece of multifunctional data acquisition card to measure control module 6.
Laser 1, beam-expanding collimation microscope group 17, dynamic self-focusing module 18, polarization splitting prism 19, quarter wave plate 20 are successively Arranged in co-axial alignment.
Beam-expanding collimation microscope group 17 can compress the angle of divergence for the scanning projection laser for coming from laser 1, and expand to connecing Convergence microscope group in nearly dynamic self-focusing module 18 expires the state of pupil, increases convergence microscope group in dynamic self-focusing module 18 Numerical aperture, and then limited scanning projection laser is irradiated to the spot size on projection undertaking region 10.In beam-expanding collimation microscope group Illumination pin hole 24 is set in 17 so that the laser that laser 1 is sent is worked in a manner of an illumination, while is eliminated veiling glare and done Disturb, improve beam quality, further reduce spot size, obtained in region 10 is accepted in projection and more preferably converge hot spot. In dynamic self-focusing module 18, focusing lens 25 is installed in accurate displacement mechanism 8, realizes the axial direction of scanning projection laser facula Self-focusing.Focusing microscope group in dynamic self-focusing module 18 is retrofocus type microscope group so that laser scanning projection's orientation distance model Enclose and reach 1~10m, still, this can cause the numerical aperture for focusing on microscope group to reduce, and about 10-3, but, due to beam-expanding collimation mirror The presence of group 17 can be made up.
In the scanning transmission light light path of polarization splitting prism 19, and twin shaft scanning galvanometer is set after quarter wave plate 20 4.Symmetrical defocus double detector light intensity detection module 21 is set in the demarcation reflected light light path of polarization splitting prism 19.With it is inclined Trap is set to converge object lens 26 and notch filter 27 in the opposite light path of the Amici prism 19 that shakes demarcation reflected light light path, for disappearing Except interference of stray light.In symmetrical defocus double detector light intensity detection module 21, in the transmission, reflected light path in Amici prism 22 Respectively be equipped with one group of convergence object lens 14, point detecting pinhole 23 and photodetector 15, point detecting pinhole 23 positioned at convergence object lens 14 with Between photodetector 15, the photosurfaces of two photodetectors 15 be respectively relative to each self-corresponding convergence object lens 14 defocus+ ΔZ、-ΔZ;The respective light intensity electrical signal of two photodetectors 15 is connected respectively to two of measurement control module 6 Light intensity input end of analog signal.The focusing driving signal output end of measurement control module 6 is connected in dynamic self-focusing module 18 Accurate displacement mechanism 8.

Claims (5)

1. a kind of self-focusing laser scanning projection device based on symmetrical defocus double detector, its part include laser (1), twin shaft scanning galvanometer (4), measurement control module (6), computer (7), computer (7) are connected with measurement control module (6); The scanning drive signal output end of measurement control module (6) is connected to the precision rotation angle mechanism (9) in twin shaft scanning galvanometer (4), The measurement control module (6) is one piece of multifunctional data acquisition card;Characterized in that, laser (1), beam-expanding collimation microscope group (17), dynamic self-focusing module (18), polarization splitting prism (19), quarter wave plate (20) sequentially coaxially arrange;In polarization spectro rib In the scanning transmission light light path of mirror (19), and twin shaft scanning galvanometer (4) is set after quarter wave plate (20);In polarization spectro rib Symmetrical defocus double detector light intensity detection module (21) is set in the demarcation reflected light light path of mirror (19);In the double detections of symmetrical defocus In device light intensity detection module (21), one group of convergence object lens (14), point are respectively equipped with the transmission, reflected light path in Amici prism (22) Detecting pinhole (23) and photodetector (15), point detecting pinhole (23) positioned at convergence object lens (14) with photodetector (15) it Between, the photosurface of two photodetectors (15) is respectively relative to each self-corresponding convergence object lens (14) defocus+Δ Z ,-Δ Z;Two The individual respective light intensity electrical signal of photodetector (15) is connected respectively to two light intensity simulation of measurement control module (6) Signal input part;The focusing driving signal output end of measurement control module (6) is connected to the essence in dynamic self-focusing module (18) Close displacement mechanism (8).
2. the self-focusing laser scanning projection device according to claim 1 based on symmetrical defocus double detector, its feature It is, beam-expanding collimation microscope group (17) can compress the angle of divergence for the scanning projection laser for coming from laser (1), and expand to connecing The state of the full pupil of convergence microscope group in nearly dynamic self-focusing module (18), increases the converging lenses in dynamic self-focusing module (18) The numerical aperture of group, and then limited scanning projection laser is irradiated to the spot size in projection undertaking region (10).
3. the self-focusing laser scanning projection device according to claim 1 based on symmetrical defocus double detector, its feature It is, illumination pin hole (24) is set in beam-expanding collimation microscope group (17) so that the laser that laser (1) is sent is with a side for illumination Formula is worked, while eliminates interference of stray light, improves beam quality, further reduces spot size, and region (10) are accepted in projection Hot spot is more preferably converged in middle acquisition.
4. the self-focusing laser scanning projection device according to claim 1 based on symmetrical defocus double detector, its feature It is, in dynamic self-focusing module (18), focusing lens (25) is installed in accurate displacement mechanism (8), realizes scanning projection The axial self-focusing of laser facula.
5. the self-focusing laser scanning projection device according to claim 1 based on symmetrical defocus double detector, its feature It is, sets trap to converge object lens (26) and trap in the light path opposite with polarization splitting prism (19) demarcation reflected light light path Wave filter (27), for eliminating interference of stray light.
CN201710992009.9A 2017-06-30 2017-10-23 Self-focusing laser scanning projection device based on symmetrical out-of-focus double detectors Active CN107765426B (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
CN201710523373 2017-06-30
CN2017105233730 2017-06-30

Publications (2)

Publication Number Publication Date
CN107765426A true CN107765426A (en) 2018-03-06
CN107765426B CN107765426B (en) 2020-10-13

Family

ID=61269026

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201710992009.9A Active CN107765426B (en) 2017-06-30 2017-10-23 Self-focusing laser scanning projection device based on symmetrical out-of-focus double detectors

Country Status (1)

Country Link
CN (1) CN107765426B (en)

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110448266A (en) * 2018-12-29 2019-11-15 中国科学院宁波工业技术研究院慈溪生物医学工程研究所 Random Laser is copolymerized focal line and scans three-dimensional ophthalmoscope and imaging method
CN111367138A (en) * 2020-04-14 2020-07-03 长春理工大学 Novel laser scanning projection device
CN111399330A (en) * 2020-04-27 2020-07-10 江西师范大学 Silicon crystal projection display screen
CN111412835A (en) * 2020-04-14 2020-07-14 长春理工大学 Novel laser scanning projection method
TWI700544B (en) * 2018-03-28 2020-08-01 宏達國際電子股份有限公司 Projection apparatus
CN111521132A (en) * 2020-04-14 2020-08-11 长春理工大学 Novel self-calibration laser scanning projection method
CN113787722A (en) * 2021-07-21 2021-12-14 武汉锐科光纤激光技术股份有限公司 Packaging device and packaging method
CN113917651A (en) * 2021-09-29 2022-01-11 中国科学院西安光学精密机械研究所 Focusing device of low-temperature optical system
CN114178679A (en) * 2020-09-15 2022-03-15 台达电子工业股份有限公司 Laser processing apparatus

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103091299A (en) * 2013-01-21 2013-05-08 北京理工大学 Laser differential confocal map microimaging imaging method and device

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103091299A (en) * 2013-01-21 2013-05-08 北京理工大学 Laser differential confocal map microimaging imaging method and device

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
李东华等: ""激光大尺度3维动态聚焦扫描加工系统研究"", 《激光技术》 *

Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI700544B (en) * 2018-03-28 2020-08-01 宏達國際電子股份有限公司 Projection apparatus
CN110448266A (en) * 2018-12-29 2019-11-15 中国科学院宁波工业技术研究院慈溪生物医学工程研究所 Random Laser is copolymerized focal line and scans three-dimensional ophthalmoscope and imaging method
CN111367138A (en) * 2020-04-14 2020-07-03 长春理工大学 Novel laser scanning projection device
CN111412835A (en) * 2020-04-14 2020-07-14 长春理工大学 Novel laser scanning projection method
CN111521132A (en) * 2020-04-14 2020-08-11 长春理工大学 Novel self-calibration laser scanning projection method
CN111412835B (en) * 2020-04-14 2021-04-30 长春理工大学 Novel laser scanning projection method
CN111399330A (en) * 2020-04-27 2020-07-10 江西师范大学 Silicon crystal projection display screen
CN114178679A (en) * 2020-09-15 2022-03-15 台达电子工业股份有限公司 Laser processing apparatus
CN113787722A (en) * 2021-07-21 2021-12-14 武汉锐科光纤激光技术股份有限公司 Packaging device and packaging method
CN113917651A (en) * 2021-09-29 2022-01-11 中国科学院西安光学精密机械研究所 Focusing device of low-temperature optical system
CN113917651B (en) * 2021-09-29 2022-10-04 中国科学院西安光学精密机械研究所 Focusing device of low-temperature optical system

Also Published As

Publication number Publication date
CN107765426B (en) 2020-10-13

Similar Documents

Publication Publication Date Title
CN107765426A (en) Self-focusing laser scanning projection device based on symmetrical defocus double detector
CN107765425B (en) Self-focusing laser scanning projection method based on symmetrical defocus double detector
CN108801178B (en) Differential confocal auto-collimation center deviation and curvature radius measuring method and device
US4473750A (en) Three-dimensional shape measuring device
CN112247382A (en) Laser welding penetration information monitoring system and method based on optical weak coherent imaging
CN107771112A (en) Probe with integrated light beam position sensor and the calibrating installation for off-line calibration
CN103675831A (en) Distance measurement apparatus
CN112748510A (en) Scanning type automatic focusing method and device with automatic leveling function
CN109187430B (en) Refractive index measuring method and device for rear-mounted pupil laser differential confocal lens
CN211876977U (en) Line focusing differential color confocal three-dimensional surface topography measuring system
CN104749901A (en) Focusing and leveling device
CN109807471A (en) A kind of laser mark printing device and method
CN115096212B (en) Three-dimensional shape measuring device and method
US20230133662A1 (en) Method for calibrating one or more optical sensors of a laser machining head, laser machining head, and laser machining system
CN116803588A (en) Welding light path system and welding method
CN111367138A (en) Novel laser scanning projection device
CN212470240U (en) Light beam pointing stability monitoring and feedback device
CN110632768B (en) Parallel Gaussian beam double telecentric system and alignment method
CN110385539A (en) Penetrating detection equipment and its detection method based on low coherence interferometry
CN104483105A (en) Interpixel crosstalk detection system and method
CN110824459B (en) Intelligent optical axis adjustment system based on interference fringes and adjustment method thereof
CN116447988B (en) Triangular laser measurement method adopting wide-spectrum light source
CN201497810U (en) Laser ranging device
CN116538956A (en) 3D measurement method based on wide spectrum light source
CN115655110A (en) Optical probe measuring head precision self-calibration method based on point self-focusing principle

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant
TR01 Transfer of patent right
TR01 Transfer of patent right

Effective date of registration: 20240724

Address after: No. 89 Fanghua Road, Hengqin New District, Zhuhai City, Guangdong Province 519000, 9th Floor, 9-011

Patentee after: Zhuhai Longying Enterprise Management Partnership Enterprise (Limited Partnership)

Country or region after: China

Address before: 130022 No. 7089 Satellite Road, Changchun, Jilin, Chaoyang District

Patentee before: CHANGCHUN University OF SCIENCE AND TECHNOLOGY

Country or region before: China

TR01 Transfer of patent right
TR01 Transfer of patent right

Effective date of registration: 20240808

Address after: Room 204, No. 863-10, Shangshengou Village, Hunnan District, Shenyang City, Liaoning Province, China

Patentee after: Shengke Liwei (Shenyang) Precision Optoelectronic Technology Co.,Ltd.

Country or region after: China

Address before: No. 89 Fanghua Road, Hengqin New District, Zhuhai City, Guangdong Province 519000, 9th Floor, 9-011

Patentee before: Zhuhai Longying Enterprise Management Partnership Enterprise (Limited Partnership)

Country or region before: China