CN206076718U - A kind of middle-infrared band optical fiber pumping/signal bundling device - Google Patents
A kind of middle-infrared band optical fiber pumping/signal bundling device Download PDFInfo
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Abstract
本实用新型的目的是提供一种中红外波段光纤抽运/信号合束器,包括信号光纤、抽运光纤、石英玻璃套管和输出光纤;所述信号光纤的纤芯材料为纯二氧化锗材料,所述光纤组束的拉锥区的拉锥比例在1~3之间;所述光纤组束与输出光纤熔接,可采用非对称电极放电加热熔接或低温熔接,信号光纤的熔接损耗低于10%;本实用新型可以实现对中红外波段激光的信号光和泵浦激光合束输出,实现高功率低损耗的信号光通过,抽运激光在光纤组束的通过率通常可以控制在98%以上,可以耦合大于百瓦的抽运激光进入输出光纤,保证高功率中红外光纤放大器的实现。
The purpose of this utility model is to provide a kind of mid-infrared band optical fiber pumping/signal beam combiner, including signal optical fiber, pumping optical fiber, quartz glass casing and output optical fiber; The fiber core material of described signal optical fiber is pure germanium dioxide Material, the tapered ratio of the tapered area of the optical fiber bundle is between 1 and 3; the optical fiber bundle and the output optical fiber can be welded by asymmetric electrode discharge heating or low temperature fusion, and the fusion loss of the signal optical fiber is low less than 10%; the utility model can realize the combined output of the signal light of the mid-infrared band laser and the pump laser, realize the passage of the signal light with high power and low loss, and the pass rate of the pump laser in the optical fiber bundle can usually be controlled at 98% % or more, it can couple pumping laser light greater than 100 watts into the output fiber to ensure the realization of high-power mid-infrared fiber amplifier.
Description
技术领域technical field
本实用新型属于光纤激光器领域,尤其涉及一种中红外波段光纤抽运/信号合束器。The utility model belongs to the field of fiber lasers, in particular to a mid-infrared band fiber pumping/signal combiner.
背景技术Background technique
中红外波段的光纤激光器近年来在气象监测、激光雷达、生物医疗、材料加工、国防安全等领域发挥着越来越重要的应用。基于非石英材料(如氟化物玻璃、碲酸盐玻璃、硫化物玻璃等)的软玻璃光纤没有石英光纤在中红外波段强烈的声子共振吸收损耗,能够支持中红外波段光纤激光的产生和低损耗传输。尤其是,近年来Er3+、Ho3+和Dy3+等稀土离子掺杂的ZBLAN光纤(氟化物光纤的一种,具体组分为ZrF4-BaF2-LaF3-AlF3-NaF)的迅速发展,使得国内外多家研究单位报道了输出功率在瓦量级的中红外激光(参见S.D.Jackson,Towards high-power mid-infrared emission from a fibre laser,Nature Photonics,6(7),423-431(2012).(S.D.Jackson,面向高功率中红外光纤激光输出,自然光电子,2012年,第6期第7卷))。这些掺杂ZBLAN光纤可以提供增益在2.7~3.1μm之间的激光辐射。但受限于软玻璃光纤的物理特性,尚缺乏基于软玻璃光纤的一系列关键光纤器件(如光纤光栅、光隔离器、光纤抽运/信号合束器、模场适配器等)和核心技术(如软玻璃光纤处理、软玻璃光纤熔接等)。这导致中红外光纤激光器研究绝大多数采用空间抽运结构,丧失了光纤激光器本应具有的结构简单、稳定性高、易于集成等优点。In recent years, fiber lasers in the mid-infrared band have played an increasingly important role in meteorological monitoring, lidar, biomedicine, material processing, national defense and security and other fields. Soft glass fibers based on non-quartz materials (such as fluoride glass, tellurite glass, sulfide glass, etc.) do not have the strong phonon resonance absorption loss of silica fibers in the mid-infrared band, and can support the generation of fiber lasers in the mid-infrared band and low loss transmission. In particular, ZBLAN fiber doped with rare earth ions such as Er 3+ , Ho 3+ and Dy 3+ in recent years (a kind of fluoride fiber, the specific composition is ZrF 4 -BaF 2 -LaF 3 -AlF 3 -NaF) The rapid development of the technology has made many domestic and foreign research institutes report mid-infrared lasers with output power in the order of watts (see SD Jackson, Towards high-power mid-infrared emission from a fiber laser, Nature Photonics, 6(7), 423- 431(2012). (SD Jackson, Towards high-power mid-infrared fiber laser output, Nature Photonics, 2012, Issue 6, Vol. 7)). These doped ZBLAN fibers can provide laser radiation with a gain between 2.7 and 3.1 μm. However, limited by the physical characteristics of soft glass optical fibers, there is still a lack of a series of key optical fiber components (such as fiber gratings, optical isolators, optical fiber pumping/signal combiners, mode field adapters, etc.) and core technologies based on soft glass optical fibers ( Such as soft glass fiber processing, soft glass fiber fusion, etc.). This has led to the vast majority of mid-infrared fiber laser research using a space-pumped structure, which loses the advantages of simple structure, high stability, and easy integration that fiber lasers should have.
近年,加拿大Laval大学报道的世界上第一个全光纤结构的Er3+掺杂3μm光纤激光器,获得了工作波长在2.94μm、平均功率达30.5W的激光输出(参见V.Fortin,M.Bernier,S.T.Bah,and R.Vallée,30W fluoride glass all-fiber laser at 2.94μm,OpticsLetter 40(12),2882-2885(2015);V.Fortin等,30W、2.94μm全光纤氟化物光纤激光器,光学快报,2015年,第40期第12卷)。然而光纤光栅带来的热以及质量下降将会限制这种直接从谐振腔输出的激光功率的进一步的提升,采用主振荡功率放大(MOPA)结构是进一步实现大功率光纤激光放大输出的常用结构,这种结构通常由振荡器和一级放大器或者更多级放大器组成。其中核心元器件为大功率光纤抽运/信号合束器,该器件可以高效率地将信号光与抽运光耦合进入的双包层增益光纤中,实现全光纤结构、高效率的激光放大输出。在多级主振荡功率放大结构中,特别要求抽运/信号合束器具有低的信号光插入损耗、高的抽运光耦合效率。目前基于MOPA结构已经实现了1μm波段单根光纤输出功率大于10KW的激光。必然地,采用MOPA结构对于中红外波段的光纤激光进行功率提升将带来更高功率的中红外激光输出。In recent years, the world's first Er 3+ doped 3 μm fiber laser with all-fiber structure reported by Laval University in Canada obtained a laser output with a working wavelength of 2.94 μm and an average power of 30.5 W (see V.Fortin, M.Bernier , STBah, and R.Vallée, 30W fluoride glass all-fiber laser at 2.94μm, OpticsLetter 40(12), 2882-2885(2015); V.Fortin et al., 30W, 2.94μm all-fiber fluoride fiber laser, Optics Letters , 2015, Issue 40, Vol. 12). However, the heat and quality degradation caused by the fiber grating will limit the further improvement of the laser power output directly from the resonator. The main oscillation power amplification (MOPA) structure is a common structure for further realizing high-power fiber laser amplification output. This structure usually consists of an oscillator and one or more stages of amplifiers. The core component is a high-power optical fiber pumping/signal combiner, which can efficiently couple signal light and pumping light into the double-clad gain fiber to achieve an all-fiber structure and high-efficiency laser amplification output . In the multi-stage main oscillation power amplification structure, the pump/signal beam combiner is particularly required to have low signal light insertion loss and high pump light coupling efficiency. At present, based on the MOPA structure, a laser with a single fiber output power greater than 10KW in the 1μm band has been realized. Inevitably, using the MOPA structure to increase the power of fiber lasers in the mid-infrared band will bring higher power mid-infrared laser output.
现有的光纤抽运/信号合束器的信号光纤、抽运光纤和输出光纤均采用石英光纤制备。由于石英光纤在波长大于2.4μm以上增强的声子共振吸收损耗,因而不能用其来传输波长位于2.4μm以上的激光信号,这也就说明现有石英光纤抽运/信号合束器无法用于中红外波段的光纤激光的放大。技术资料显示,目前尚无任何关于中红外波段的光纤抽运/信号合束器的任何设计与报道。The signal optical fiber, pumping optical fiber and output optical fiber of the existing optical fiber pumping/signal combiner are all made of silica optical fiber. Due to the enhanced phonon resonance absorption loss of the quartz fiber at a wavelength greater than 2.4 μm, it cannot be used to transmit laser signals with a wavelength above 2.4 μm, which means that the existing quartz fiber pump/signal combiner cannot be used Amplification of fiber lasers in the mid-infrared region. According to the technical information, there is no design or report about the optical fiber pumping/signal combiner in the mid-infrared band.
实用新型内容Utility model content
本实用新型的目的是提供一种信号光损耗低、抽运光耦合效率高的中红外波段光纤抽运/信号合束器。The purpose of the utility model is to provide a mid-infrared band optical fiber pumping/signal combiner with low loss of signal light and high coupling efficiency of pumping light.
为解决上述技术问题,本实用新型采用以下技术方案:In order to solve the above technical problems, the utility model adopts the following technical solutions:
一种中红外波段光纤抽运/信号合束器,该抽运/信号合束器包括信号光纤、抽运光纤、石英玻璃套管和输出光纤。所述信号光纤的一端与所述抽运光纤的一端从石英玻璃套管的同一端插入并固定,进行熔融拉锥,结合为一带有拉锥区(包含锥区和腰区)的光纤组束;在腰区位置对光纤组束进行切割,切割面与所述光纤组束的几何中心线垂直,将切割后的光纤组束与所述输出光纤通过熔接连接。A mid-infrared band optical fiber pumping/signal combiner includes a signal optical fiber, a pumping optical fiber, a quartz glass sleeve and an output optical fiber. One end of the signal optical fiber and one end of the pumping optical fiber are inserted and fixed from the same end of the quartz glass sleeve, melted and tapered, and combined into an optical fiber bundle with a tapered region (including a tapered region and a waist region) ; cutting the optical fiber bundle at the waist region, the cutting plane is perpendicular to the geometric center line of the optical fiber bundle, and connecting the cut optical fiber bundle with the output optical fiber through fusion splicing.
所述信号光纤的纤芯材料为纯二氧化锗材料,包层材料为二氧化锗和石英混合材料或者纯石英材料。The core material of the signal optical fiber is pure germanium dioxide material, and the cladding material is a mixed material of germanium dioxide and quartz or pure quartz material.
所述信号光纤为单包层结构光纤。The signal optical fiber is a single-clad optical fiber.
所述信号光纤的纤芯支持2.7~3.1μm的单模或少模激光传输,信号光纤的纤芯数值孔径可以有效将激光约束在纤芯内部,保证低损耗传输。The core of the signal fiber supports single-mode or few-mode laser transmission of 2.7-3.1 μm, and the numerical aperture of the core of the signal fiber can effectively confine the laser inside the core to ensure low-loss transmission.
所述信号光纤的纤芯直径范围为2.5~30μm,包层直径范围为125~300μm,光纤纤芯直径的选取使得其支持的激光模场面积与中红外信号激光器的输出光纤支持激光模场面积相同。The core diameter of the signal optical fiber ranges from 2.5 to 30 μm, and the cladding diameter ranges from 125 to 300 μm. The fiber core diameter is selected so that the laser mode field area supported by it is the same as the laser mode field area supported by the output fiber of the mid-infrared signal laser. same.
所述抽运光纤与中红外光纤放大器抽运激光器的耦合光纤类型相同。The pumping fiber is of the same type as the coupling fiber of the mid-infrared fiber amplifier pumping laser.
所述抽运光纤为多模石英光纤,光纤数量可以为6根或者18根,所述抽运光纤可以支持793nm,或者976nm,或者1150nm、或者1550nm激光的传输。The pumping fiber is a multimode silica fiber, and the number of fibers can be 6 or 18. The pumping fiber can support the transmission of 793nm, or 976nm, or 1150nm, or 1550nm laser.
所述输出光纤为非掺杂双包层氟化物光纤,光纤的纤芯和包层均为氟化物玻璃材料,光纤的纤芯数值孔径在0.15~0.35之间,包层数值孔径在0.4~0.7之间。The output optical fiber is a non-doped double-clad fluoride optical fiber, the core and cladding of the optical fiber are made of fluoride glass, the numerical aperture of the core of the optical fiber is between 0.15 and 0.35, and the numerical aperture of the cladding is between 0.4 and 0.7 between.
所述输出光纤的纤芯直径范围为2.5~30μm,外包层直径范围为125~600μm,内包层直径范围为100~300μm,内包层直径小于外包层直径,具体选择的纤芯和包层直径与中红外光纤放大器所需的稀土掺杂增益光纤的纤芯和包层直径相同。The core diameter of the output optical fiber ranges from 2.5 to 30 μm, the outer cladding diameter ranges from 125 to 600 μm, the inner cladding diameter ranges from 100 to 300 μm, and the inner cladding diameter is smaller than the outer cladding diameter. The core and cladding diameters of rare-earth-doped gain fibers required for mid-infrared fiber amplifiers are the same.
本实用新型中,将抽运光纤和信号光纤的一端剥除涂覆层后,插入一根石英玻璃管中,其中抽运光纤均匀排布在信号光纤周围;所述抽运光纤、信号光纤、石英玻璃套管的中轴线相互平行。然后将插有光纤的石英玻璃管进行熔融拉锥结合为一带有拉锥区的光纤组束。In the utility model, after the coating layer is stripped off one end of the pumping optical fiber and the signal optical fiber, they are inserted into a quartz glass tube, wherein the pumping optical fiber is evenly arranged around the signal optical fiber; the pumping optical fiber, signal optical fiber, The central axes of the quartz glass sleeves are parallel to each other. Then, the quartz glass tube inserted with the optical fiber is fused and tapered to form a bundle of optical fibers with a tapered region.
本实用新型中,所述光纤组束的拉锥区的输入端(石英玻璃管被插入光纤的一端)与输出端(与输出光纤熔接处)处的横截面的外切圆直径之比为拉锥比例,其值一般在1~3之间,拉锥区长度的选取要满足信号光纤和抽运光纤在拉锥过程中无拉锥损耗这一条件。In the utility model, the ratio of the diameter of the circumscribed circle of the cross section at the input end (the end where the quartz glass tube is inserted into the optical fiber) and the output end (the place where the output optical fiber is welded) of the tapered region of the optical fiber bundle is drawn The taper ratio, its value is generally between 1 and 3, and the selection of the length of the tapered region should meet the condition that the signal fiber and the pump fiber have no tapered loss during the tapering process.
本实用新型中,光纤组束在拉锥区的腰区处横截面的外切圆直径小于或等于输出光纤直径。In the utility model, the diameter of the circumscribed circle of the cross section of the optical fiber bundle at the waist region of the tapered region is smaller than or equal to the diameter of the output optical fiber.
本实用新型中,所述光纤组束在与所述输出光纤通过端面熔接之前,需执行加热扩芯操作,扩芯后信号光纤在光纤组束末端的模场直径与输出光纤的纤芯直径相同。In the utility model, before the fiber bundle is fused with the output fiber through the end face, heating and core expansion operations need to be performed, and the mode field diameter of the signal fiber at the end of the fiber bundle after core expansion is the same as the core diameter of the output fiber .
本实用新型中,所述光纤组束与输出光纤熔接,可采用非对称电极放电加热熔接或低温熔接,信号光纤的熔接损耗低于10%,抽运光的通过率在98%以上。In the utility model, the welding of the optical fiber bundle and the output optical fiber can adopt asymmetric electrode discharge heating welding or low temperature welding, the welding loss of the signal optical fiber is less than 10%, and the passing rate of the pumping light is above 98%.
与现有光纤抽运/信号合束器技术相比,本实用新型的有益效果在于:Compared with the existing optical fiber pumping/signal combiner technology, the utility model has the beneficial effects of:
1.本实用新型可以实现对中红外波段激光的信号光和泵浦激光合束输出,其信号光纤为二氧化锗光纤,可以支持波长在2.7~3.1μm的低损耗传输,输出光纤为双包层氟化物光纤,可以与后续掺杂氟化物光纤进行熔接连接;1. The utility model can realize the combined output of the signal light and the pump laser of the mid-infrared band laser. The signal fiber is a germanium dioxide fiber, which can support low-loss transmission with a wavelength of 2.7-3.1 μm. The output fiber is double-wrapped One-layer fluoride optical fiber, which can be fusion-spliced with the subsequent doped fluoride optical fiber;
2.本实用新型的光纤组束中信号光纤在组束完成后可以进行加热扩芯,使得其模场直径最终于输出光纤的纤芯直径相匹配,可以保证信号激光低损耗的通过该光纤抽运/信号合束器,实现高功率低损耗的信号光通过。2. In the fiber bundle of the present invention, the signal fiber can be heated and core expanded after the bundle is completed, so that the mode field diameter finally matches the core diameter of the output fiber, which can ensure that the signal laser is pumped through the fiber with low loss. The transport/signal beam combiner realizes the passage of high-power and low-loss signal light.
3.本实用新型的光纤组束中拉锥比例的选取,主要依据是保证抽运激光在光纤组束(拉锥区域)的高通过率,通过率通常可以控制在98%以上;由于信号光纤和抽运光纤参数的不同,信号光纤插入损耗的控制主要是光纤组束后的热扩芯技术来保证的。3. The selection of the tapering ratio in the optical fiber bundle of the present utility model is mainly based on ensuring the high pass rate of the pumping laser in the fiber bundle (taper region), and the pass rate can be controlled above 98% usually; due to the signal optical fiber Different from the parameters of the pumping fiber, the control of the insertion loss of the signal fiber is mainly guaranteed by the thermal core expansion technology after the fiber is bundled.
4.本实用新型的抽运光纤为石英多模光纤,可以支持793nm,或者976nm,或者1150nm,或者1550nm的激光传输,具体的激光波长的选取与输出光纤接续的增益光纤的吸收谱决定。由于目前这些波长处的半导体激光器和光纤激光器的输出功率都可以达到数十瓦量级,因此通过本光纤抽运/信号束器,至少可以耦合大于百瓦的抽运激光进入输出光纤,保证高功率中红外光纤放大器的实现。4. The pumping fiber of the present utility model is a quartz multimode fiber, which can support 793nm, or 976nm, or 1150nm, or 1550nm laser transmission, and the selection of the specific laser wavelength is determined by the absorption spectrum of the gain fiber connected to the output fiber. Since the output power of semiconductor lasers and fiber lasers at these wavelengths can reach the order of tens of watts, through this optical fiber pump/signal beamer, at least pumping lasers greater than 100 watts can be coupled into the output fiber to ensure high Realization of a power mid-infrared fiber amplifier.
附图说明Description of drawings
为了更清楚地说明本实用新型实施例或现有技术中的技术方案,下面将对实施例或现有技术描述中所需要使用的附图作简单地介绍,显而易见地,下面描述中的附图仅仅是本实用新型的一些实施例,对于本领域普通技术人员来讲,在不付出创造性劳动性的前提下,还可以根据这些附图获得其他的附图。In order to more clearly illustrate the technical solutions in the embodiments of the present invention or the prior art, the following will briefly introduce the accompanying drawings that need to be used in the description of the embodiments or the prior art. Obviously, the accompanying drawings in the following description These are only some embodiments of the utility model, and those skilled in the art can also obtain other drawings according to these drawings without any creative effort.
图1是本实用新型实施例中拉锥后的光纤组束的剖面主视示意图;Fig. 1 is the cross-sectional front schematic diagram of the optical fiber group bundle after tapering in the utility model embodiment;
图2是本实用新型实施例的中红外光纤抽运/信号合束器的剖面主视示意图;Fig. 2 is a cross-sectional schematic diagram of a mid-infrared optical fiber pumping/signal combiner according to an embodiment of the present invention;
图3为图2中A-A处的剖面示意图;Fig. 3 is a schematic cross-sectional view at A-A in Fig. 2;
图4为图2中B-B处的剖面示意图;Fig. 4 is a schematic cross-sectional view at B-B in Fig. 2;
图5为图2中C-C处的剖面示意图;Fig. 5 is a schematic cross-sectional view at C-C in Fig. 2;
图例说明:illustration:
1、信号光纤;2、抽运光纤;3、石英套管;4、输出光纤;5、锥区;6、腰区;7、腰区切割位置;21~26、抽运光纤;8、腰区等效光纤;81、腰区等效光纤包层;82、腰区等效光纤纤芯;41、输出光纤包层;42、输出光纤纤芯。1. Signal optical fiber; 2. Pumping optical fiber; 3. Quartz sleeve; 4. Output optical fiber; 5. Cone area; 6. Waist area; 7. Cutting position of waist area; 81. Equivalent optical fiber cladding in waist area; 82. Equivalent optical fiber core in waist area; 41. Output optical fiber cladding; 42. Output optical fiber core.
具体实施方式detailed description
下面将结合本实用新型实施例中的附图,对本实用新型实施例中的技术方案进行清楚、完整地描述,显然,所描述的实施例仅仅是本实用新型一部分实施例,而不是全部的实施例。基于本实用新型中的实施例,本领域普通技术人员在没有作出创造性劳动前提下所获得的所有其他实施例,都属于本实用新型保护的范围。The technical solutions in the embodiments of the present invention will be clearly and completely described below in conjunction with the accompanying drawings in the embodiments of the present invention. Obviously, the described embodiments are only part of the embodiments of the present invention, not all of them. example. Based on the embodiments of the present utility model, all other embodiments obtained by persons of ordinary skill in the art without making creative efforts belong to the scope of protection of the present utility model.
如图1所示的实施例中,所述输入信号光纤1的一端与所述抽运光纤2的一端插入石英玻璃套管3固定后,进行熔融拉锥结合为一带有拉锥区(包含锥区5和腰区6)的光纤组束。并在腰区位置7处对光纤组束进行垂直切割,然后将切割后的光纤组束与输出光纤4通过端面熔接相连接,得到一种如图2所示的中红外波段光纤抽运/信号合束器。In the embodiment shown in Figure 1, one end of the input signal optical fiber 1 and one end of the pumping optical fiber 2 are inserted into the quartz glass sleeve 3 and fixed, and then melted and bonded into a tapered region (comprising a tapered Fiber bundles in Zone 5 and Waist Zone 6). And vertically cut the optical fiber bundle at position 7 in the waist region, and then connect the cut optical fiber bundle with the output optical fiber 4 through end face fusion to obtain a mid-infrared band optical fiber pumping/signal as shown in Figure 2 Combiner.
本实施例中将1根信号光纤1和6根抽运光纤21~26的涂覆层材料去除后组束插入石英玻璃管3中,确保输入信号光纤1位于光纤组束的中心,其横截面如图3所示;并将光纤组束加热至熔融状态进行拉锥,拉锥比例为2,锥区5的长度为1cm;当光纤组束的外径大小为250μm时,减小加热强度,当腰区长度为5mm时停止加热和拉锥过程。光纤组束中拉锥比例的选取,可以保证抽运激光在光纤组束(拉锥区域)的通过率为99%。拉锥完成后的光纤组束如图1所示。In this embodiment, the coating materials of one signal optical fiber 1 and six pumping optical fibers 21-26 are removed and then bundled and inserted into the quartz glass tube 3 to ensure that the input signal optical fiber 1 is located in the center of the optical fiber bundle. As shown in Figure 3; and the optical fiber bundle is heated to a molten state for tapering, the tapering ratio is 2, and the length of the tapered region 5 is 1cm; when the outer diameter of the optical fiber bundle is 250 μm, reduce the heating intensity, The heating and tapering process was stopped when the length of the waist region was 5 mm. The selection of the tapered ratio in the optical fiber bundle can ensure that the pass rate of the pumping laser in the optical fiber bundle (the tapered region) is 99%. The fiber bundle after tapering is shown in Figure 1.
本实施例中对石英玻璃套管3拉锥时,信号光纤1的纤芯直径按等比例变小,在腰区6处信号光纤1的纤芯直径仅为5μm;为了与接续的输出光纤4实现低损耗信号光通过,需要对腰区6进行加热扩芯处理;采用氢氧焰对腰区6进行加热,加热时间为20分钟,加热后腰区6处信号光纤1的纤芯中的二氧化锗扩芯进入包层中增加了纤芯模场面积大小,使得锥区的位置7处信号光纤模场面积与输出光纤4的纤芯模场面积相等。降低信号激光通过该光纤抽运/信号合束器的损耗,实现高功率低损耗的信号光通过。In this embodiment, when the quartz glass sleeve 3 is tapered, the core diameter of the signal optical fiber 1 becomes smaller in proportion, and the core diameter of the signal optical fiber 1 at the waist region 6 is only 5 μm; To realize the passage of low-loss signal light, the waist region 6 needs to be heated and core expanded; the waist region 6 is heated with an oxyhydrogen flame for 20 minutes, and two of the cores of the signal optical fiber 1 at the waist region 6 are heated. Expanding the core of germanium oxide into the cladding increases the size of the core mode field area, making the mode field area of the signal fiber at position 7 of the taper region equal to the core mode field area of the output fiber 4 . Reduce the loss of the signal laser passing through the optical fiber pumping/signal combiner, and realize the passage of high-power and low-loss signal light.
本实施例中,加热扩芯结束后在腰区6的中间位置7处对拉锥后的光纤组束进行垂直切割;切割位置7处的光纤组束形成了腰区等效光纤8,其截面如图4所示。腰区等效光纤8的横截面结构由等效光纤包层81和腰区等效光纤纤芯82组成。其中信号光纤1的包层、抽运光纤21~26和玻璃套管3在加热拉锥过后形成了腰区等效光纤8的等效光纤包层81。拉锥后的信号光纤1的纤芯再经加热扩芯后形成等效光纤纤芯82。In this embodiment, after heating and expanding the core, the tapered optical fiber bundle is vertically cut at the middle position 7 of the waist region 6; the fiber bundle at the cutting position 7 forms an equivalent optical fiber 8 in the waist region, and its cross-section As shown in Figure 4. The cross-sectional structure of the equivalent optical fiber 8 in the waist region is composed of an equivalent optical fiber cladding 81 and an equivalent optical fiber core 82 in the waist region. The cladding of the signal optical fiber 1, the pumping optical fibers 21-26 and the glass sleeve 3 form the equivalent optical fiber cladding 81 of the equivalent optical fiber 8 in the waist region after heating and tapering. The core of the tapered signal optical fiber 1 is heated and expanded to form an equivalent optical fiber core 82 .
本实施例中,光纤组束与输出光纤4在切割位置7处采用温熔接技术进行熔接,得到本实用新型提供的中红外波段光纤抽运/信号合束器。In this embodiment, the optical fiber bundle and the output optical fiber 4 are fused at the cutting position 7 using warm fusion technology to obtain the mid-infrared band optical fiber pumping/signal combiner provided by the utility model.
本实施例中信号光纤1为单包层结构光纤,其纤芯材料为纯二氧化锗材料,可以支持波长在2.7~3.1μm的低损耗传输。包层材料为纯石英材料,纤芯/包层直径为10μm/125μm。In this embodiment, the signal optical fiber 1 is a single-clad optical fiber, and its core material is pure germanium dioxide, which can support low-loss transmission with a wavelength of 2.7-3.1 μm. The cladding material is pure quartz material, and the core/cladding diameter is 10μm/125μm.
石英玻璃套管3的内径为400μm,外径为500μm。The inner diameter of the quartz glass sleeve 3 is 400 μm, and the outer diameter is 500 μm.
输出光纤4为非掺杂双包层氟化物光纤,纤芯和内包层均为氟化物玻璃材料,可以与后续掺杂氟化物光纤进行熔接连接。纤芯/内包层直径分别为20μm/250μm,纤芯/包层数值孔径分别为0.27/0.46;输出光纤4的外包层为丙烯酸树脂材料的涂覆层,直径为450μm;涂覆层材料去除之后的光纤横截面图如图5所示,其中41为输出光纤内包层,42为输出光纤纤芯。The output optical fiber 4 is a non-doped double-clad fluoride optical fiber, the core and the inner cladding of which are made of fluoride glass, and can be fusion-spliced with subsequent doped fluoride optical fibers. The diameter of the core/inner cladding is 20 μm/250 μm, and the numerical aperture of the core/cladding is 0.27/0.46; the outer cladding of the output fiber 4 is a coating layer of acrylic resin material, and the diameter is 450 μm; after the coating material is removed The cross-sectional view of the optical fiber is shown in Figure 5, wherein 41 is the inner cladding of the output optical fiber, and 42 is the core of the output optical fiber.
抽运光纤2为纤芯/包层直径为105μm/125μm的多模石英光纤,光纤的纤芯数值孔径为0.15,光纤数量为6根。多模石英光纤可以支持793nm,或者976nm,或者1150nm,或者1550nm的激光传输,具体的激光波长的选取与输出光纤接续的增益光纤的吸收谱决定。由于目前这些波长处的半导体激光器和光纤激光器的输出功率都可以达到数十瓦量级,因此通过本光纤抽运/信号束器,至少可以耦合大于百瓦的抽运激光进入输出光纤,保证高功率中红外光纤放大器的实现。The pumping fiber 2 is a multimode silica fiber with a core/cladding diameter of 105 μm/125 μm, a core numerical aperture of the fiber is 0.15, and the number of fibers is 6. Multimode silica fiber can support 793nm, or 976nm, or 1150nm, or 1550nm laser transmission, the specific laser wavelength selection is determined by the absorption spectrum of the gain fiber connected to the output fiber. Since the output power of semiconductor lasers and fiber lasers at these wavelengths can reach the order of tens of watts, through this optical fiber pump/signal beamer, at least pumping lasers greater than 100 watts can be coupled into the output fiber to ensure high Realization of a power mid-infrared fiber amplifier.
以上所述,仅为本实用新型的具体实施方式,但本实用新型的保护范围并不局限于此,任何熟悉本技术领域的技术人员在本实用新型揭露的技术范围内,可轻易想到的变化或替换,都应涵盖在本实用新型的保护范围之内。因此,本实用新型的保护范围应该以权利要求书的保护范围为准。The above is only a specific embodiment of the utility model, but the scope of protection of the utility model is not limited thereto, and any skilled person familiar with the technical field can easily think of changes within the technical scope disclosed in the utility model Or replacement, all should be covered within the scope of protection of the present utility model. Therefore, the protection scope of the present utility model should be based on the protection scope of the claims.
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CN108919419A (en) * | 2018-07-25 | 2018-11-30 | 珠海光库科技股份有限公司 | Bundling device and preparation method thereof |
TWI662305B (en) * | 2018-10-18 | 2019-06-11 | 搏盟科技股份有限公司 | Optical fiber bundling structure and manufacturing method thereof |
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CN106253038A (en) * | 2016-08-31 | 2016-12-21 | 中国人民解放军国防科学技术大学 | A kind of middle-infrared band optical fiber pumping/signal bundling device |
CN108919419A (en) * | 2018-07-25 | 2018-11-30 | 珠海光库科技股份有限公司 | Bundling device and preparation method thereof |
TWI662305B (en) * | 2018-10-18 | 2019-06-11 | 搏盟科技股份有限公司 | Optical fiber bundling structure and manufacturing method thereof |
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