CN203241622U - Ribbon beam generation device - Google Patents

Ribbon beam generation device Download PDF

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Publication number
CN203241622U
CN203241622U CN 201320141622 CN201320141622U CN203241622U CN 203241622 U CN203241622 U CN 203241622U CN 201320141622 CN201320141622 CN 201320141622 CN 201320141622 U CN201320141622 U CN 201320141622U CN 203241622 U CN203241622 U CN 203241622U
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CN
China
Prior art keywords
cylindrical mirror
ribbon beam
generation device
beam generation
collimation lens
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.)
Expired - Fee Related
Application number
CN 201320141622
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Chinese (zh)
Inventor
徐建程
王飞舟
陈达如
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Zhejiang Normal University CJNU
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Zhejiang Normal University CJNU
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Priority to CN 201320141622 priority Critical patent/CN203241622U/en
Application granted granted Critical
Publication of CN203241622U publication Critical patent/CN203241622U/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

The utility model provides a ribbon beam generation device. The ribbon beam generation device comprises a laser device, a first cylindrical mirror, a second cylindrical mirror and a collimation lens, wherein the generatrices of the first cylindrical mirror and the second cylindrical mirror are mutually vertical, and the conjugate distances of the first cylindrical mirror and the second cylindrical mirror are equal. The device is capable of shaping approximately circular light spots emitted by the laser device into a ribbon beam, and the ribbon beam has the characteristics of wavefront collimation and uniform energy distribution. The ribbon beam generation device is simple in structure, high in energy utilization rate, and capable of being applied to the fields of internal defect detection for optical components, and the like.

Description

The ribbon beam generation device
Technical field
The utility model relates to the applied optics field, is specifically related to a kind of ribbon beam generation device.
Background technology
The defective of optical element is one of principal element that causes optical element laser damage.How effectively detecting the inherent vice of optical element, also is the underlying issue that must solve in the optics secondary industry.The inherent vice of optical element does not also have ripe detection method and the checkout equipment of moulding at present.Some researchists have carried out preliminary research to the detection of internal defect of optical element, the main inherent vice that adopts the method measurement optical element of laser scanning, the illuminating bundle that adopts is banded collimation uniform beam, the hot spot rectangular in shape of namely throwing light on, a length of side is much larger than another length of side.The easiest method of expecting is to make the slit of a correspondence, obtain ribbon beam through behind the slit after illuminating bundle expands, but the capacity usage ratio of the method is too low.In order to improve capacity usage ratio, have the scholar once to adopt the method for optical grating diffraction to obtain ribbon beam, but the light beam behind the optical grating diffraction normally disperse or assemble, when being used for the scanning survey internal defect of optical element, can have a negative impact to accuracy of detection.Internal defect of optical element detects required ribbon beam, require the approximate collimation of its wavefront, energy distribution even, and higher capacity usage ratio is arranged, existing method and the device that produces ribbon beam can not satisfy the requirement that internal defect of optical element detects effectively.
The utility model content
In order to overcome above-mentioned the deficiencies in the prior art, the utility model provides a kind of ribbon beam generation device, but the ribbon beam that this device produce power is evenly distributed, wavefront collimates, capacity usage ratio is high can satisfy the requirement that internal defect of optical element detects.
The technical scheme that the utility model patent adopts is: the ribbon beam generation device comprises laser instrument, the first cylindrical mirror, the second cylindrical mirror and collimation lens; Wherein the bus of the first cylindrical mirror and the second cylindrical mirror is orthogonal, and conjugate distance equates.The spot shaping of the sub-circular that this device can send laser instrument becomes wavefront collimation, the uniform ribbon beam of energy distribution.Described ribbon beam generation device is simple in structure, and capacity usage ratio is high, may be used on the fields such as internal defect of optical element detection.
Compare with grating Diffraction Method with traditional slit method, the ribbon beam that device that the utility model provides produces have energy distribution evenly, wavefront collimation, capacity usage ratio advantages of higher.
Description of drawings
Fig. 1 is the synoptic diagram of the embodiment of ribbon beam generation device of the present utility model;
Fig. 2 is that ribbon beam generation device of the present utility model is in the floor map of yz direction;
Fig. 3 is that ribbon beam generation device of the present utility model is in the floor map of xz direction;
Among the figure: 1 is laser instrument, and 2 is the first cylindrical mirror, and 3 is the second cylindrical mirror, and 4 is collimation lens.
Embodiment
Shown in Figure 1 is the synoptic diagram of the embodiment of ribbon beam generation device of the present utility model.The beam shaping system that this device comprises LASER Light Source 1 and is arranged at this LASER Light Source light direction.Described beam shaping system comprises the first cylindrical mirror 2, the second cylindrical mirror 3 and the collimation lens 4 that sets gradually along same optical axis (z axle).The first cylindrical mirror 2 is mutual vertical with the second cylindrical mirror 3 buses and conjugate distance is equal, and the front focus of described collimation lens 4 overlaps with the back focus of described the second cylindrical mirror 3.The light that laser instrument 1 sends is by described the first cylindrical mirror 2 and 3 incidents of the second cylindrical mirror, and by described collimation lens 4 outgoing.
Shown in Figure 2 is the floor map of Fig. 1 on the yz direction.If the light beam that laser instrument 1 sends is b at the window size of y direction, the first cylindrical mirror 2 with described light beam at the y direction focusing to F point (this moment the second cylindrical mirror 3 be flat-panel component in the equivalence of y direction), then collimated outgoing by collimation lens 4.If the first cylindrical mirror 2 is f at the focal length of y direction 2, the focal length of collimation lens 4 is f 4, then the outgoing collimated light beam is bf at the beamwidth of y direction 4/ f 2
Shown in Figure 3 is the floor map of Fig. 1 on the xz direction.If the light beam that laser instrument 1 sends is a at the window size of x direction, the first cylindrical mirror 2 is flat-panel component in the equivalence of x direction, the second cylindrical mirror 3 with light beam at the x direction focusing to the F point; Then by collimation lens 4 collimation outgoing.If the second cylindrical mirror 3 is f at the focal length of x direction 4, then the outgoing collimated light beam is af at the beamwidth of x direction 4/ f 3
Therefore, described the first cylindrical mirror 2 and the second cylindrical mirror 3 focus on the F point with whole light beam.The front focus of collimation lens 4 overlaps with the F point, can obtain the collimated light beam that energy even distributes after focusing on the beam collimation of focal point F by this collimation lens 4, and the hot spot of its formation is respectively af in the size of x and y direction 4/ f 3And bf 4/ f 2Focal distance f by appropriate design the first cylindrical mirror 2, the second cylindrical mirror 3, collimation lens 4 2, f 3And f 4, just can obtain the ribbon beam of required size.With the plated surface anti-reflection film of the first cylindrical mirror 2, the second cylindrical mirror 3 and collimation lens 4, just can realize that the capacity usage ratio of beam shaping system is greater than 90%.
In the present embodiment, the employing wavelength is that 532nm, power are the diode pumped solid state laser of 400mW.The light beam window that laser instrument 1 sends is a=2mm and b=2mm; The focal distance f of the first cylindrical mirror 2 2=25mm, the focal distance f of the second cylindrical mirror 3 3=5mm, the focal distance f of collimation lens 4 4=50mm, the banded collimated light beam of outgoing is respectively 4mm and 20mm in the size of x and y direction after the shaping.

Claims (1)

1. a ribbon beam generation device is characterized in that, comprises laser instrument, the first cylindrical mirror, the second cylindrical mirror and collimation lens; Wherein the bus of the first cylindrical mirror and the second cylindrical mirror is orthogonal, and conjugate distance equates; The back focus of the first cylindrical mirror and the second cylindrical mirror overlaps with the front focus of collimation lens.
CN 201320141622 2013-03-15 2013-03-15 Ribbon beam generation device Expired - Fee Related CN203241622U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN 201320141622 CN203241622U (en) 2013-03-15 2013-03-15 Ribbon beam generation device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN 201320141622 CN203241622U (en) 2013-03-15 2013-03-15 Ribbon beam generation device

Publications (1)

Publication Number Publication Date
CN203241622U true CN203241622U (en) 2013-10-16

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Family Applications (1)

Application Number Title Priority Date Filing Date
CN 201320141622 Expired - Fee Related CN203241622U (en) 2013-03-15 2013-03-15 Ribbon beam generation device

Country Status (1)

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CN (1) CN203241622U (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103971672A (en) * 2014-04-29 2014-08-06 浙江大学 Underwater laser sound source with control directivity and control method thereof
CN110416872A (en) * 2019-07-31 2019-11-05 天津大学 Radian and the tunable arc beam delivery system of width
WO2020239129A1 (en) * 2019-05-30 2020-12-03 西安精英光电技术有限公司 Combined lens-based line laser homogenization generation apparatus

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103971672A (en) * 2014-04-29 2014-08-06 浙江大学 Underwater laser sound source with control directivity and control method thereof
CN103971672B (en) * 2014-04-29 2017-01-04 浙江大学 Control underwater laser sound source and the control method thereof of directivity
WO2020239129A1 (en) * 2019-05-30 2020-12-03 西安精英光电技术有限公司 Combined lens-based line laser homogenization generation apparatus
US11960097B2 (en) 2019-05-30 2024-04-16 Elite Optoelectronics Co., Ltd Combined lenses-based apparatus for line laser uniformity generation
CN110416872A (en) * 2019-07-31 2019-11-05 天津大学 Radian and the tunable arc beam delivery system of width

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C17 Cessation of patent right
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20131016

Termination date: 20140315