CN207588207U - A kind of beam quality reforming unit - Google Patents
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- CN207588207U CN207588207U CN201721746309.0U CN201721746309U CN207588207U CN 207588207 U CN207588207 U CN 207588207U CN 201721746309 U CN201721746309 U CN 201721746309U CN 207588207 U CN207588207 U CN 207588207U
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- 238000002407 reforming Methods 0.000 title claims abstract 6
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 claims abstract description 39
- 238000005086 pumping Methods 0.000 claims abstract description 29
- 239000000835 fiber Substances 0.000 claims abstract description 25
- 239000000377 silicon dioxide Substances 0.000 claims abstract description 19
- 239000004065 semiconductor Substances 0.000 claims abstract description 16
- 230000005281 excited state Effects 0.000 claims abstract description 4
- 230000009466 transformation Effects 0.000 claims abstract description 3
- 229910052769 Ytterbium Inorganic materials 0.000 claims abstract 6
- NAWDYIZEMPQZHO-UHFFFAOYSA-N ytterbium Chemical compound [Yb] NAWDYIZEMPQZHO-UHFFFAOYSA-N 0.000 claims abstract 6
- JBRZTFJDHDCESZ-UHFFFAOYSA-N AsGa Chemical compound [As]#[Ga] JBRZTFJDHDCESZ-UHFFFAOYSA-N 0.000 claims description 3
- 229910001218 Gallium arsenide Inorganic materials 0.000 claims description 3
- 238000006243 chemical reaction Methods 0.000 abstract description 18
- 238000000034 method Methods 0.000 abstract description 4
- 230000005855 radiation Effects 0.000 abstract 1
- 230000006735 deficit Effects 0.000 description 4
- 235000012239 silicon dioxide Nutrition 0.000 description 3
- 239000013078 crystal Substances 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000005516 engineering process Methods 0.000 description 2
- 239000011159 matrix material Substances 0.000 description 2
- 238000001816 cooling Methods 0.000 description 1
- 238000013461 design Methods 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 230000005283 ground state Effects 0.000 description 1
- 230000017525 heat dissipation Effects 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 239000013307 optical fiber Substances 0.000 description 1
- 239000010453 quartz Substances 0.000 description 1
- 238000011160 research Methods 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
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Abstract
Description
技术领域technical field
本实用新型涉及全固态激光器领域,具体涉及到一种光束质量转化装置领域。The utility model relates to the field of all-solid-state lasers, in particular to the field of a light beam quality conversion device.
背景技术Background technique
由于掺Yb3+激光介质通常受到严重的热效应的限制,高功率、高光束质量、高转化效率全固态激光器进展缓慢。如今随着同带泵浦技术的出现,基于半导体激光器和碟片激光器的同带泵浦的Yb:YAG激光器正成为获得高功率、高光束质量、高转化效率的全固态激光器的研究热点。Yb3+掺杂的Yb:YAG浓度可达20%,通过利用940nm波长的泵浦光进行泵浦,YAG:YAG晶体可以发射中心波长为1050nm和1030nm两个主要激光波长。通过利用碟片激光器的高效散热性,可将全固态激光器热量进行分担,将极小的热量带到同带泵浦的掺镱石英光纤中,从而实现具有低量子亏损(2%以内)的同带泵浦激光器,并获得高功率近衍射极限M2<2的激光输出。Since the Yb 3+ doped laser medium is usually limited by severe thermal effects, the development of all-solid-state lasers with high power, high beam quality, and high conversion efficiency is slow. Nowadays, with the emergence of in-band pumping technology, Yb:YAG lasers based on the in-band pumping of semiconductor lasers and disk lasers are becoming a research hotspot for obtaining all-solid-state lasers with high power, high beam quality, and high conversion efficiency. The concentration of Yb:YAG doped with Yb 3+ can reach 20%. By pumping with 940nm wavelength pump light, YAG:YAG crystal can emit two main laser wavelengths with central wavelengths of 1050nm and 1030nm. By using the high-efficiency heat dissipation of the disk laser, the heat of the all-solid-state laser can be shared, and a very small amount of heat can be brought to the ytterbium-doped silica fiber pumped with the same band, so as to achieve a simultaneous laser with low quantum deficit (within 2%) It is equipped with a pump laser and obtains a high-power near-diffraction-limited M 2 <2 laser output.
实用新型内容Utility model content
本实用新型的目的在于提供一种光束质量转化装置,利用半导体激光器和碟片激光器作为一、二级泵浦源,同带泵浦Yb3+掺杂的光纤增益介质,其量子效率极高,光束质量接近衍射极限的激光输出,而且能很好的解决热效应问题,同时输出激光为光纤输出单模激光。The purpose of this utility model is to provide a beam quality conversion device, which uses semiconductor lasers and disk lasers as primary and secondary pumping sources, and pumps Yb 3+ doped fiber gain media with the same belt, and its quantum efficiency is extremely high. The beam quality is close to the laser output of the diffraction limit, and it can solve the thermal effect problem well, and the output laser is a single-mode laser output by the fiber.
所述的半导体激光器,采用中心波长为940nm、969nm砷化镓激光器作为一级泵浦源。Said semiconductor laser adopts gallium arsenide laser with center wavelength of 940nm and 969nm as the primary pumping source.
一种光束质量转化装置,包括半导体激光器,碟片激光器,掺镱石英光纤组成;半导体激光器作为一级泵浦源的泵浦激光进入碟片激光器对碟片激光器进行泵浦,获得具有高光-光(70%以上)转化效率的多模激光输出;利用碟片激光器输出的激光,作为二级泵浦源对掺镱石英光纤进行同带泵浦(量子亏损<2%),经掺镱石英光纤后输出,实现了高光束质量(M2<2)的转化装置。A beam quality conversion device, including a semiconductor laser, a disk laser, and an ytterbium-doped silica fiber; the semiconductor laser is used as a primary pumping source, and the pumping laser enters the disk laser to pump the disk laser to obtain a high-light (above 70%) multi-mode laser output with conversion efficiency; use the laser output from the disk laser as a secondary pump source to pump the ytterbium-doped silica fiber in the same band (quantum deficit <2%), and pass the ytterbium-doped silica fiber After the output, a conversion device with high beam quality (M 2 <2) is realized.
所述的碟片激光器,采用24、32、48冲程碟片激光器作为二级泵浦源。增益介质为Yb:YAG;碟片激光器输出激光器为多模激光,其输出波长为1030nm、1050nm;The said disk laser adopts 24, 32, 48 stroke disk lasers as the secondary pumping source. The gain medium is Yb:YAG; the output laser of the disk laser is a multimode laser, and its output wavelength is 1030nm and 1050nm;
所述的掺镱石英光纤,其增益介质为Yb3+,掺杂的基质为二氧化硅,经过二级泵浦后的激光器的输出波长为1080nm;光纤增益介质Yb3+掺杂摩尔浓度15-20%。In the ytterbium-doped silica fiber, the gain medium is Yb 3+ , the doped matrix is silicon dioxide, and the output wavelength of the laser after secondary pumping is 1080 nm; the fiber gain medium Yb 3+ is doped at a molar concentration of 15 -20%.
所述的第一级半导体泵浦源光束质量M2<200,二级泵浦碟片激光器光束质量M2<50,最后获得的掺镱石英光纤可获得光束质量M2<2的高光束质量的激光输出。The beam quality of the first-stage semiconductor pumping source M 2 <200, the beam quality of the second-stage pumping disk laser M 2 <50, and the finally obtained ytterbium-doped silica fiber can obtain a high beam quality of M 2 <2 laser output.
本实用新型提供的一种光束质量转化装置,该装置采用模块化设计,结构简单,易于维护。The utility model provides a light beam quality conversion device, which adopts a modular design, has a simple structure and is easy to maintain.
附图说明Description of drawings
图1为实施例1的一种光束质量转化装置Fig. 1 is a kind of beam quality transformation device of embodiment 1
具体实施方式Detailed ways
为了使本实用新型的目的及优点更加清楚明白,以下结合具体实施例对本实用新型进行进一步详细说明。应当理解,此处所描述的具体实施例仅用以解释本实用新型,并不用于限定本实用新型。该具体实施例以一种光束质量转化装置及方法进行解释说明。In order to make the purpose and advantages of the utility model clearer, the utility model will be further described in detail below in conjunction with specific embodiments. It should be understood that the specific embodiments described here are only used to explain the utility model, and are not intended to limit the utility model. The specific embodiment is explained with a beam quality conversion device and method.
如图1所示,一种光束质量转化装置,包括半导体激光器1,碟片激光器3,掺镱石英光纤5组成。其特征在于:半导体激光器1作为一级泵浦源对碟片激光器3进行泵浦2,获得具有高光-光(70%)转化效率的多模激光输出;利用碟片激光器3输出的激光,作为二级泵浦源对掺镱石英光纤进行同带泵浦4(量子亏损<2%),实现了高光束质量(M2<2)的转化装置。As shown in FIG. 1 , a beam quality conversion device includes a semiconductor laser 1 , a disk laser 3 , and an ytterbium-doped silica fiber 5 . It is characterized in that: the semiconductor laser 1 is used as a primary pump source to pump 2 the disk laser 3 to obtain a multi-mode laser output with high light-to-light (70%) conversion efficiency; the laser output by the disk laser 3 is used as The secondary pump source pumps the ytterbium-doped silica fiber in-band 4 (quantum deficit<2%), realizing a conversion device with high beam quality (M2<2).
所述的半导体激光器1采用中心波长为940nm、969nm砷化镓激光器作为一级泵浦源,其阵列或者为单管形式。Said semiconductor laser 1 uses gallium arsenide lasers with center wavelengths of 940nm and 969nm as the first-stage pumping source, and its array or single-tube form.
所述的碟片激光器3采用24、32、48冲程碟片激光器3作为二级泵浦源。增益介质为Yb:YAG;碟片激光器3输出激光器为多模激光,其输出波长为1030nm、1050nm;The disk laser 3 uses 24, 32, 48 stroke disk lasers 3 as the secondary pumping source. The gain medium is Yb:YAG; the output laser of the disk laser 3 is a multimode laser, and its output wavelength is 1030nm and 1050nm;
所述的碟片激光器3主要包括:反射棱镜和非球面反射聚焦镜,其中反射棱镜用来转折泵浦光,实现多冲程泵浦碟片晶体的目的。非球面反射聚焦镜是利用平行光如何到其反射面后聚焦于焦点位置的特性的反射元件。The disk laser 3 mainly includes: a reflective prism and an aspheric reflective focusing mirror, wherein the reflective prism is used to deflect the pump light to achieve the purpose of multi-stroke pumping the disk crystal. The aspherical reflective focusing mirror is a reflective element that utilizes the characteristics of how parallel light reaches its reflective surface and then focuses on the focal point.
所述的掺镱石英光纤5增益介质为Yb3+,掺杂的基质为二氧化硅,经过二级泵浦后的激光器的输出波长为1080nm;光纤增益介质Yb3+掺杂浓度15-20%,该同带泵浦范围可获得极高的光-光转化效率,理论光-光转化效率可达98%,该系统光-光转化效率可达70%以上,是实现光束质量转化的重要环节。由于其具有的高量子效率98%,仅为2%的量子亏损,其可输出超高功率激光器,同时仅会产生极少的热量。通过利用微通道冷却技术即可将该热量散失掉。The gain medium of the ytterbium-doped silica fiber 5 is Yb3+, the doped matrix is silicon dioxide, and the output wavelength of the laser after secondary pumping is 1080nm; the Yb3+ doping concentration of the fiber gain medium is 15-20%, the same The pump range can obtain extremely high light-to-light conversion efficiency, the theoretical light-to-light conversion efficiency can reach 98%, and the light-to-light conversion efficiency of the system can reach more than 70%, which is an important link to realize the beam quality conversion. Due to its high quantum efficiency of 98% and only 2% quantum deficit, it can output ultra-high power lasers while generating very little heat. This heat is dissipated by utilizing micro-channel cooling technology.
所述的一种光束质量转化装置及方法,第一级半导体泵浦源1光束质量M2<200,二级泵浦碟片激光器3光束质量M2<50,最后同带泵浦4获得的掺镱石英光纤5可获得光束质量M2<2的高光束质量的激光输出。The beam quality conversion device and method, the beam quality M2<200 of the first-stage semiconductor pump source 1, the beam quality M2<50 of the second-stage pumping disk laser 3, and finally the ytterbium-doped The quartz optical fiber 5 can obtain high beam quality laser output with beam quality M2<2.
所述装置中,1030nm同带泵浦碟片激光器3作为1050nm掺镱石英光纤5的同带泵浦源,通过光纤波分复用器耦合进入掺镱石英光纤5,基态能级吸收1030nm泵浦从能级2F7/2跃迁至高能级2F5/2,从激发态2F5/2跃迁至2F7/2,这种准三能级结构中会产生1050nm的光子。1050nm激光的产生是通过使用长度很短的高掺杂的掺镱光纤和窄带光纤布拉格光栅实现的,由于激光纵模间距与激光腔腔长相关,减少激光腔腔长可以增大激光纵模间距,利于单纵模的选取,而窄带光纤布拉格光栅可以进一步限制输出激光的波长范围,最终获得窄线宽1050nm单频激光输出。In the device, the 1030nm co-band pumping disk laser 3 is used as the co-band pumping source of the 1050nm ytterbium-doped silica fiber 5, coupled into the ytterbium-doped silica fiber 5 through a fiber wavelength division multiplexer, and the ground state energy level absorbs the 1030nm pumping source. Transition from the energy level 2F7/2 to the higher energy level 2F5/2, and from the excited state 2F5/2 to 2F7/2, will generate photons at 1050nm in this quasi-three-level structure. The generation of 1050nm laser is achieved by using a very short length of highly doped ytterbium-doped fiber and a narrow-band fiber Bragg grating. Since the laser longitudinal mode spacing is related to the laser cavity length, reducing the laser cavity length can increase the laser longitudinal mode spacing. , which is conducive to the selection of single longitudinal mode, and the narrow-band fiber Bragg grating can further limit the wavelength range of the output laser, and finally obtain a single-frequency laser output with a narrow linewidth of 1050nm.
以上所述仅是本实用新型的优选实施方式,应当指出,对于本技术领域的普通技术人员来说,在不脱离本实用新型原理的前提下,还可以做出若干改进和润饰,这些改进和润饰也应视为本实用新型的保护范围。The above is only a preferred embodiment of the utility model, it should be pointed out that for those of ordinary skill in the art, without departing from the principle of the utility model, some improvements and modifications can also be made, these improvements and Retouching should also be regarded as the scope of protection of the present utility model.
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