CN202383362U - Polarization rotation device and laser polarization beam combiner system - Google Patents
Polarization rotation device and laser polarization beam combiner system Download PDFInfo
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- CN202383362U CN202383362U CN2011205346313U CN201120534631U CN202383362U CN 202383362 U CN202383362 U CN 202383362U CN 2011205346313 U CN2011205346313 U CN 2011205346313U CN 201120534631 U CN201120534631 U CN 201120534631U CN 202383362 U CN202383362 U CN 202383362U
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Abstract
The utility model discloses a polarization rotation device and a laser polarization beam combiner system, belonging to the technical field of laser. The polarization rotation device comprises two reflecting mirrors, and the incident planes of the same incident light in the two reflecting mirrors are perpendicular to each other. The system comprises two laser components 1 and 2 having the same polarization state, a polarization rotation device and a polarization beam combiner; the polarization rotation device is arranged in front of the output end of the laser component 1 for reflecting the optical axis of the laser component 1, for outputting light beams, to a beam combining input side of the polarization beam combiner; the optical axis of the laser component 2 for outputting light beams is intersected with another beam combining input side of the polarization beam combiner; and the optical axes of the two laser components on the polarization beam combiner are equally high. Compared with the prior art, the device provided by the utility model has the advantages of smaller structural volume, lower cost and the like.
Description
Technical field
The utility model provides a kind of polarization rotation device and laser instrument polarization to close beam system, utilizes this system can carry out the polarization coupled of semiconductor laser, realizes the merging output of two-way laser instrument, belongs to laser technology field.
Background technology
Advantages such as as everyone knows, semiconductor laser is little because of its volume, electricity conversion is high and the life-span is long are widely used in every field.Especially the high power semiconductor lasers of high light beam quality, high brightness all has a wide range of applications and bigger development prospect in fields such as Solid State Laser pumping, materials processing, laser medicine, fiber laser pumping sources.
At present,, adopt the spatial beam complex method mostly, utilize catoptron, wavelength bundling device and polarization beam combiner to realize the merging of light beam for realizing the output of high power semiconductor lasers.Polarization closes the general dual mode that adopts of bundle: a kind of is that the two-way semiconductor laser that is used to be coupled has different polarization states, and one is that S attitude polarized light one is P attitude polarized light, and two-way light impinges perpendicularly on the polarization beam combiner each other; The second way is that the two-way semiconductor laser that is used to be coupled has identical polarization state; Place half-wave plate therein before one road laser instrument its polarization state is changed, incide on the polarization beam combiner after S attitude polarized light is become P attitude polarized light or P attitude polarized light become S attitude polarized light.In first method; Can directly use two kinds of semiconductor lasers with different output polarization attitudes; Also can be directly No. one semiconductor laser be wherein revolved and turn 90 degrees; Make S attitude polarized light become P attitude polarized light or P attitude polarized light becomes S attitude polarized light, but can increase the volume of total system like this, this problem is especially remarkable when being used for laser assembly that polarization closes bundle and being array or module.In the second approach; Use half-wave plate directly S attitude polarized light to be converted into P attitude polarized light, can use the semiconductor laser elements of identical polarization state, simple in structure and system bulk is little; But the half-wave plate processing cost is high, and its processing, installation accuracy can have a strong impact on and close Shu Xiaoguo.
The utility model content
The purpose of the utility model is to overcome to have now closes the defective among the Shu Fangfa, provides a kind of polarization rotation device of advantages of simple more and laser instrument polarization to close beam system.
The technical scheme of the utility model is:
A kind of polarization rotation device is characterized in that comprising two catoptrons 3,4, and the plane of incidence of same incident light in two catoptrons 3,4 is orthogonal.
Further, said catoptron is the reflecting surface of plane mirror or reflecting prism.
A kind of laser instrument polarization closes beam system, it is characterized in that comprising that two have laser assembly 1,2, one polarization rotation devices of identical polarization state, a polarization beam combiner; Laser assembly 1 output terminal the place ahead is provided with one makes the optical axis of laser assembly 1 output beam reflex to the polarization rotation device that said polarization beam combiner one closes the bundle input side; The optical axis of laser assembly 2 output beams meets at said polarization beam combiner, and another closes the bundle input side, height such as two-laser assembly optical axis on said polarization beam combiner; Wherein, said polarization rotation device comprises two catoptrons 3,4, and the plane of incidence of same incident light in two catoptrons 3,4 is orthogonal.
Further, said laser assembly front end is provided with fast axis collimation lens or slow axis collimation lens or fast and slow axis collimation lens.
Further, two said laser assemblies be installed on respectively heat sink on; Said laser assembly is the single tube semiconductor laser, or semiconductor laser array, or comprises the semiconductor laser module of a plurality of single tube laser instruments or array.
Further, said polarization beam combiner is PBS prism or Glan Taylor prism or diaphragm type plain film or natural birefringence crystal.
Further; Said laser assembly 2 output terminal the place aheads be provided with one make the optical axis of laser assembly 2 output beams reflex to said polarization beam combiner another closes the catoptron 5 of bundle input side, the optical axis height after said catoptron 5 reflections equates with the optical axis height that said polarization rotation device reflects.
The utility model utilizes the kine bias of reflecting prism to change the change that characteristic realizes polarization state.Its principle is as shown in Figure 1; Adopt two catoptrons ( parts 3,4 among the figure) to constitute one group of space image rotation parts, the plane of incidence of promptly same incident light in catoptron 3,4 is orthogonal; In the process of light beam through this parts propagation; Along with the deflection of emergent light axis, in the plane vertical with optical axis, as direction can deflect thereupon.Fig. 1 has indicated the deflection of incident space coordinates in the beam propagation process, has provided the deflection state of reflection back coordinate axis each time.This structure is used for the image planes deflection of imaging system mostly.The polarization state of supposing the semiconductor laser output beam is the polarization direction linearly polarized light consistent with slow-axis direction; Be also referred to as S attitude polarized light; And semiconductor laser is a strip hot spot (launching spot 7 of first catoptron) behind the fast and slow axis collimation, that is to say that its linear polarization is consistent with the rectangular direction of hot spot, behind two secondary reflections; The beam direction of semiconductor laser deflects; Become vertical strip (the outgoing hot spot 8 of second catoptron) from the horizontal strip shape, its polarization direction is also revolved thereupon and is turn 90 degrees, and becomes P attitude linearly polarized light from S attitude linearly polarized light.
Adopt structure as shown in Figure 2; Two same wave appearance with the warp of polarization state in advance the semiconductor laser elements of collimation (parts 1 among the figure; 2) the vertical placement; And it is poor to have certain height between the two, incides on the polarization beam combiner 6 with the P polarization state behind the image rotation parts that the S attitude polarized light of low level semiconductor laser elements 1 passes through to be made up of two catoptrons ( parts 3,4 among the figure); Incide on the polarization beam combiner 6 after high-order semiconductor laser elements 2 is turned back through the 3rd catoptron 5, two bundle laser are merged into a branch of output.Turning back of 5 pairs of light paths of catoptron can effectively reduce the volume of total system.
Compare with existing method, the good effect of the utility model is:
The utility model has been realized the conversion of laser beam polarization state through utilizing one group of space image rotation parts, can replace expensive device such as existing half-wave plate, has practiced thrift cost; Advantages such as be easy to adjustment with time space image rotation parts, to close Shu Fangfa simpler thereby make, and is easy to realize, it is littler to the utlity model has structural volume, and cost is lower.
Description of drawings
Fig. 1. the schematic diagram of polarization rotation device;
(a) front elevation, (b) side view;
Fig. 2. novel semi-conductor laser instrument polarization closes the synoptic diagram of beam system;
Among the figure: 1. low level semiconductor laser elements, 2. high-order semiconductor laser elements, 3. first catoptron, 4. second catoptron, 5. the 3rd catoptron, 6. polarization beam combiner, the 7. launching spot of first catoptron, 8. the outgoing hot spot of second catoptron.
Embodiment
In conjunction with Fig. 2, the utility model method is elaborated.
1. (parts 1 among the figure through the semiconductor laser elements of collimation in advance for two identical polarization states; 2) the vertical placement; And have certain height poor (that is: this difference in height can make the height of parts 5 output optical axis and the height such as optical axis of parts 4 outputs) between the two, the output facula of the two is S attitude linearly polarized light 7 shown in Figure 1.
2. the S attitude polarized light of low level semiconductor laser elements 1 is through (parts 3 among the figure by two catoptrons; 4) behind the image rotation parts that constitute with 8 outgoing of P polarization state; The position and the angle of two catoptrons of adjustment; Make the height of output optical axis and the height such as optical axis of high-order semiconductor laser 2, and output beam is P attitude linearly polarized light completely.
3. in the output light path of second catoptron 4, place polarization beam combiner 6, the adjustment light path makes that the output optical axis of polarization beam combiner 6 and second catoptron 4 is vertical and the laser output power of maximum is arranged.
4. in the output light path of high-order semiconductor laser 2, place the 3rd catoptron 5; Output optical axis turned back incide on the polarization beam combiner 6 behind the special angle; Adjust the 3rd catoptron 5, the laser output power that makes two-beam be merged into a branch of output and have maximum through polarization beam combiner 6.
Claims (7)
1. a polarization rotation device is characterized in that comprising two catoptrons (3), (4), and the plane of incidence of same incident light in catoptron (3), (4) is orthogonal.
2. polarization rotation device as claimed in claim 1 is characterized in that said catoptron is the reflecting surface of plane mirror or reflecting prism.
3. a laser instrument polarization closes beam system, it is characterized in that comprising that two have laser assembly (1), (2) of identical polarization state, a polarization rotation device, a polarization beam combiner; Laser assembly (1) output terminal the place ahead is provided with one makes the optical axis of laser assembly (1) output beam reflex to the polarization rotation device that said polarization beam combiner one closes the bundle input side; The optical axis of laser assembly (2) output beam meets at said polarization beam combiner, and another closes the bundle input side, height such as two-laser assembly optical axis on said polarization beam combiner; Wherein, said polarization rotation device comprises two catoptrons (3), (4), and the plane of incidence of same incident light in catoptron (3), (4) is orthogonal.
4. laser instrument polarization as claimed in claim 3 closes beam system, it is characterized in that said laser assembly front end is provided with fast axis collimation lens or slow axis collimation lens or fast and slow axis collimation lens.
5. close beam system like claim 3 or 4 described laser instrument polarizations, it is characterized in that two said laser assemblies be installed on respectively heat sink on; Said laser assembly is the single tube semiconductor laser, or semiconductor laser array, or comprises the semiconductor laser module of a plurality of single tube laser instruments or array.
6. laser instrument polarization as claimed in claim 3 closes beam system, it is characterized in that said polarization beam combiner is PBS prism or Glan Taylor prism or diaphragm type plain film or natural birefringence crystal.
7. laser instrument polarization as claimed in claim 3 closes beam system; It is characterized in that said laser assembly (2) output terminal the place ahead be provided with one make the optical axis of laser assembly (2) output beam reflex to said polarization beam combiner another closes the catoptron (5) of bundle input side, the optical axis height after said catoptron (5) reflection equates with the optical axis height that said polarization rotation device reflects.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN2011205346313U CN202383362U (en) | 2011-11-22 | 2011-12-19 | Polarization rotation device and laser polarization beam combiner system |
Applications Claiming Priority (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201120467663 | 2011-11-22 | ||
| CN201120467663.6 | 2011-11-22 | ||
| CN2011205346313U CN202383362U (en) | 2011-11-22 | 2011-12-19 | Polarization rotation device and laser polarization beam combiner system |
Publications (1)
| Publication Number | Publication Date |
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| CN202383362U true CN202383362U (en) | 2012-08-15 |
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| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN2011104283716A Pending CN102566075A (en) | 2011-11-22 | 2011-12-19 | Polarization rotating device as well as polarization beam combining method and system of laser |
| CN2011205346313U Expired - Lifetime CN202383362U (en) | 2011-11-22 | 2011-12-19 | Polarization rotation device and laser polarization beam combiner system |
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| Application Number | Title | Priority Date | Filing Date |
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| CN2011104283716A Pending CN102566075A (en) | 2011-11-22 | 2011-12-19 | Polarization rotating device as well as polarization beam combining method and system of laser |
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| CN (2) | CN102566075A (en) |
Cited By (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102566075A (en) * | 2011-11-22 | 2012-07-11 | 北京凯普林光电科技有限公司 | Polarization rotating device as well as polarization beam combining method and system of laser |
| CN109346917A (en) * | 2018-12-05 | 2019-02-15 | 中国电子科技集团公司第五十三研究所 | A kind of conjunction beam system based on quantum cascade laser |
| CN112130339A (en) * | 2020-09-29 | 2020-12-25 | 苏州众为光电有限公司 | Laser polarization beam combination system |
| WO2021051469A1 (en) * | 2019-09-18 | 2021-03-25 | 深圳市星汉激光科技股份有限公司 | Semiconductor laser |
| CN112904581A (en) * | 2021-02-05 | 2021-06-04 | 西安炬光科技股份有限公司 | Laser module, device, optical space conversion method and medium-intensity light spot forming method |
| CN117767101A (en) * | 2024-02-20 | 2024-03-26 | 深圳市星汉激光科技股份有限公司 | Small-size laser and laser equipment |
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| US20180100635A1 (en) * | 2016-10-07 | 2018-04-12 | Christie Digital Systems Usa, Inc. | Apparatus for combining light beams |
| CN106932785B (en) * | 2017-02-27 | 2019-11-05 | 南京红露麟激光雷达科技有限公司 | A kind of time-multiplexed polarization coherent Doppler wind-observation laser radar |
| CN107015375A (en) * | 2017-04-27 | 2017-08-04 | 中国科学院长春光学精密机械与物理研究所 | A kind of laser polarization coupling light path debugging device and method |
| CN114006269A (en) * | 2021-12-29 | 2022-02-01 | 深圳市星汉激光科技股份有限公司 | Direct output system of high-power semiconductor laser and polarization beam combining structure thereof |
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| JPS52150A (en) * | 1975-06-21 | 1977-01-05 | Ando Electric Co Ltd | Square root extracting device |
| JPH0461677A (en) * | 1990-06-27 | 1992-02-27 | Nec Corp | Optical disk medium |
| JPH052150A (en) * | 1991-06-24 | 1993-01-08 | Nippon Avionics Co Ltd | Polarized light source device |
| JPH1144864A (en) * | 1997-05-30 | 1999-02-16 | Fuji Photo Optical Co Ltd | Illumination optical system for liquid crystal display device |
| CN1774596A (en) * | 2003-06-09 | 2006-05-17 | 微阳有限公司 | A light pipe based projection engine |
| CN201199288Y (en) * | 2007-11-14 | 2009-02-25 | 中国科学院长春光学精密机械与物理研究所 | Light beam coupling apparatus capable of implementing high-power semiconductor laser array using rectangular prism set |
| CN101782689A (en) * | 2010-01-26 | 2010-07-21 | 金世龙 | Method for completely converting natural light into linear polarized light vibrating unidirectionally and application |
| CN101854030A (en) * | 2010-05-04 | 2010-10-06 | 长春德信光电技术有限公司 | Laser light source device of high-power semiconductor |
| CN102566075A (en) * | 2011-11-22 | 2012-07-11 | 北京凯普林光电科技有限公司 | Polarization rotating device as well as polarization beam combining method and system of laser |
-
2011
- 2011-12-19 CN CN2011104283716A patent/CN102566075A/en active Pending
- 2011-12-19 CN CN2011205346313U patent/CN202383362U/en not_active Expired - Lifetime
Cited By (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102566075A (en) * | 2011-11-22 | 2012-07-11 | 北京凯普林光电科技有限公司 | Polarization rotating device as well as polarization beam combining method and system of laser |
| CN109346917A (en) * | 2018-12-05 | 2019-02-15 | 中国电子科技集团公司第五十三研究所 | A kind of conjunction beam system based on quantum cascade laser |
| WO2021051469A1 (en) * | 2019-09-18 | 2021-03-25 | 深圳市星汉激光科技股份有限公司 | Semiconductor laser |
| CN112130339A (en) * | 2020-09-29 | 2020-12-25 | 苏州众为光电有限公司 | Laser polarization beam combination system |
| CN112130339B (en) * | 2020-09-29 | 2022-08-12 | 苏州众为光电有限公司 | Laser polarization beam combination system |
| CN112904581A (en) * | 2021-02-05 | 2021-06-04 | 西安炬光科技股份有限公司 | Laser module, device, optical space conversion method and medium-intensity light spot forming method |
| CN117767101A (en) * | 2024-02-20 | 2024-03-26 | 深圳市星汉激光科技股份有限公司 | Small-size laser and laser equipment |
| CN117767101B (en) * | 2024-02-20 | 2024-05-07 | 深圳市星汉激光科技股份有限公司 | Small-size laser and laser equipment |
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| CN102566075A (en) | 2012-07-11 |
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Legal Events
| Date | Code | Title | Description |
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| C14 | Grant of patent or utility model | ||
| GR01 | Patent grant | ||
| C56 | Change in the name or address of the patentee | ||
| CP01 | Change in the name or title of a patent holder |
Address after: 100070, Beijing, Fengtai District science and Technology Park, Feng Feng Road, No. 4, 6 Patentee after: BWT BEIJING LTD. Address before: 100070, Beijing, Fengtai District science and Technology Park, Feng Feng Road, No. 4, 6 Patentee before: BWT Beijing Ltd. |
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| PE01 | Entry into force of the registration of the contract for pledge of patent right |
Denomination of utility model: Polarization rotation device and laser polarization beam combiner system Effective date of registration: 20171219 Granted publication date: 20120815 Pledgee: Beijing good faith financing Company limited by guarantee Pledgor: BWT BEIJING LTD. Registration number: 2017990001099 |
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| PE01 | Entry into force of the registration of the contract for pledge of patent right | ||
| PC01 | Cancellation of the registration of the contract for pledge of patent right |
Date of cancellation: 20190705 Granted publication date: 20120815 Pledgee: Beijing good faith financing Company limited by guarantee Pledgor: BWT BEIJING LTD. Registration number: 2017990001099 |
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| PC01 | Cancellation of the registration of the contract for pledge of patent right | ||
| CX01 | Expiry of patent term |
Granted publication date: 20120815 |
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| CX01 | Expiry of patent term |