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1.
掺Yb3+双包层光纤激光器的数值分析   总被引:17,自引:7,他引:10  
本文对976nm激光泵浦掺Yb3+双包层光纤激光器进行了数值模拟,分析了泵浦光及激光在光纤中的分布、输出功率与泵浦功率的关系、光纤长度及腔镜反射率对输出激光功率的影响,所得结论与实验现象基本一致.  相似文献   

2.
端面泵浦掺Yb3+双包层光纤激光器   总被引:1,自引:0,他引:1       下载免费PDF全文
从双包层光纤激光器的速率方程出发,得到了光纤中泵浦光与激光的功率分布、输出功率与泵浦功率的关系、腔镜反射率及光纤长度对输出功率的影响。研究结果表明:输出激光功率与光纤长度及后腔镜反射率有很强的依赖关系,存在一个输出功率最大的最佳光纤长度。后腔镜反射率越大,输出激光功率越小;当光纤长度较短时,在输出端放置反射镜使泵浦光高反射,可以提高输出功率和效率。通过对端面泵浦掺Yb3+双包层光纤激光器进行理论分析和实验研究,得到输出激光的中心波长为1088.3nm,斜率效率为33.7%,最大输出功率为1.75W。  相似文献   

3.
掺Yb3+光纤激光器的特性与设计   总被引:2,自引:2,他引:0       下载免费PDF全文
 从速率方程出发,对波长为980nm的激光泵浦掺Yb3+光纤激光器进行数值模拟,全面分析激光器阈值功率、输出激光功率、增益等重要参数与泵浦功率、光纤长度、腔镜反射率、掺杂浓度等参量之间的关系。采用高浓度掺Yb3+光纤对环形光纤激光器做了初步实验研究,所得结论与实验模拟结果基本一致。  相似文献   

4.
对线形腔LD泵浦掺镱的双包层光纤激光器进行研究,通过数值模拟,分析了不同泵浦方式下的泵浦光、激光输出功率和增益特性在光纤中的分布。结果表明,单端后向泵浦输出功率率较高,对于小功率光纤激光器则是最佳选择。进一步又研究了单端后向对称泵浦输出功率与光纤长度及腔镜反射率的影响,为提高光纤激光器的输出功率提供了理论和实验依据。  相似文献   

5.
基于光纤光栅谐振腔的掺镱全光纤激光器设计(英文)   总被引:1,自引:0,他引:1  
采用数值分析方法分析了光纤长度、后腔镜反射率等因素对激光器输出阈值泵浦功率、输出功率的影响,为全光纤激光器的优化设计提供了理论基础.在设计过程中采用光纤光栅作为光纤激光器的反馈与选频腔镜,通过锥度光纤实现了泵浦模块与掺镱双包层光纤之间的低损耗连接以及高效率的泵浦激光功率传输,成功研制了具备稳定窄化线宽激光输出的掺镱全光纤激光器.实验得到了波长峰值在1 082 .50 nm,谱线宽度0 .113 nm,最大输出功率8 .5 W,泵浦阈值功率0 .8 W,斜率效率为70 .8 %的稳定激光输出.  相似文献   

6.
首先从掺铥光纤激光器的速率方程和光传输方程出发,建立数学模型,通过Matlab软件进行数值计算,分析了泵浦光和激光沿光纤的分布以及各能级离子数的变化。在不同掺杂浓度下,研究了小信号增益与入纤泵浦功率的关系以及泵浦光和激光功率与增益介质长度的关系。在不同泵浦功率下,研究了输出功率与输出耦合镜反射率的关系。进一步对不同泵浦吸收系数,研究了斜率效率和泵浦阈值与光纤长度的关系。分析结果表明:存在最佳光纤长度和最佳耦合输出透过率,使得激光输出功率达到最佳值。  相似文献   

7.
首先从掺铥光纤激光器的速率方程和光传输方程出发,建立数学模型,通过Matlab软件进行数值计算,分析了泵浦光和激光沿光纤的分布以及各能级离子数的变化.在不同掺杂浓度下,研究了小信号增益与入纤泵浦功率的关系以及泵浦光和激光功率与增益介质长度的关系.在不同泵浦功率下,研究了输出功率与输出耦合镜反射率的关系.进一步对不同泵浦吸收系数,研究了斜率效率和泵浦阈值与光纤长度的关系.分析结果表明存在最佳光纤长度和最佳耦合输出透过率,使得激光输出功率达到最佳值.  相似文献   

8.
对强泵浦下线形腔掺Yb3+双包层光纤激光器输出特性进行了理论和实验研究。通过数值模拟,分析了泵浦光及激光在光纤中的分布、输出功率与泵浦功率的关系、光纤长度及腔镜反射率对激光输出功率的影响。在实验中,利用D型掺Yb3+双包层光纤获得了输出功率10 6W的光纤激光输出,斜率效率达86%。测量了在不同输出耦合条件下的输出功率、阈值泵浦功率和斜率效率,理论分析与实验结果基本一致,为进一步提高光纤激光器功率提供了理论和实验依据。  相似文献   

9.
15W光子晶体光纤激光器的研究   总被引:4,自引:1,他引:3  
利用光子晶体光纤在原来输出功率3 4W的基础上,研制成功了激光输出15W的光子晶体光纤激光器,实验装置为典型的F P腔结构,分别采用二色镜和光纤端面作为高反射腔镜和激光输出腔镜 一端二色镜紧贴光纤的入射端面,它对1 0 5 μm~1 1μm波段信号光的反射率大于99% ,对976nm泵浦光透射率为93% ;另一端利用光纤端面4 %Fresnel反射作为输出端反馈与二相色镜构成了线形谐振腔 实验采用掺Yb3+ 双包层光子晶体光纤,长度为2 0m 内包层为2 0 0 μm ,外包层为380 μm ,Yb2 O3浓度为1 5mol % 当泵浦功率为6 0W时,获得了15W 1 1μm的激光输出 15W光…  相似文献   

10.
光子晶体光纤放大器增益特性的实验研究   总被引:1,自引:1,他引:0  
 采用掺Yb3+双包层光子晶体光纤作为放大器的增益介质,在双端泵浦方式下,理论并实验研究了不同信号光时放大器的增益特性。在双端泵浦方式下,泵浦总功率为150.2 W、信号光功率为6 W时,获得了72 W的功率输出,斜率效率达到了60%。实验发现当泵浦总功率超过一定值时,由光纤端面反射形成的振荡腔引起放大器寄生振荡,并由于各种非线性效应出现了自脉动现象,影响了输出功率的进一步提高。  相似文献   

11.
A high efficient LD (laser diode) pumped Tm3+ doped double clad silica fiber laser with an intravacity biconical taper was reported. A biconical taper located ~3 cm from the output end of the fiber laser was fabricated by heating and stretching method with a length 1.5 cm and waist diameter ~20 µm. The slope efficiency was 49.8% with respected to the launched pump power, and the maximum output power was 1.97 W. Pre and post output laser power ratio was ~10. This fiber laser was compared with other three biconical tapered fiber lasers (the same fiber with different tapers) and a uniform geometry fiber laser. With intracavity biconical tapers, fiber lasers’ thresholds were ~1 W higher than the fiber laser without the taper (1.97 W). The pump end’s slope efficiencies of fiber lasers with tapers were 3–5% in contrast with 37.6% of the uniform one. After tapered, the pre and post laser power ratios were much higher than the un-tapered one’s, but not changed much with the launched pump power.  相似文献   

12.
Zhu X  Jain R 《Optics letters》2007,32(1):26-28
We report on >9W transverse-fundamental-mode CW output near 3 mum from a 4m heavily erbium-doped ZBLAN double-clad fiber laser pumped by a collimated 100 W 975 nm laser diode array. The pump threshold of the fiber laser was about 1W, and the slope efficiency was 21.3%. The peak wavelength of free running was about 2708 nm at low pump power and moved to around 2785 nm at high pump power. Output of 9W was obtained when the launched pump power was 42.8W. The output, however, fluctuated intensively like a pulsed laser, and the operation broke down with optical damage of the pumping end facet when the pump was increased beyond 42.8 W. Therefore, alleviation of the operation fluctuation, heat management, and strengthening the pumping fiber are crucial considerations for the stable operation of 10-W-level mid-IR ZBLAN fiber lasers.  相似文献   

13.
采用国产大模场面积双包层光纤的714W连续光纤激光器   总被引:33,自引:2,他引:31  
采用两个中心波长约976 nm准直输出的高功率半导体激光模块为抽运源,通过空间滤波和非球面透镜耦合技术,双端抽运长度为21 m的大模场面积国产掺镱双包层光纤,获得了714.5 W的高功率连续激光输出。采用反向抽运,当入纤抽运功率为760 W时,激光输出功率达到501 W;采用双端抽运,当入纤抽运功率为1137 W时,获得了714.5 W的高功率连续输出,光光转换效率为62.8%,斜率效率为67%。  相似文献   

14.
基于光纤光栅的高功率光纤激光器   总被引:7,自引:3,他引:4  
分析了光纤光栅的选频原理以及光纤光栅基高功率光纤激光器的阈值特性和输出特性.采用紫外写入的光纤光栅做谐振腔,研制了全光纤结构的高功率光纤激光器,泵浦阈值为186 mW, 最大输出功率1.78 W,斜率效率59%,实验结果与理论分析基本吻合.  相似文献   

15.
Efficient and stable continuous-wave (CW) laser operation at 1053 nm in a Nd-doped phosphate single-mode fiber (Nd:PSMF) has been demonstrated experimentally. The fiber laser consisted of a 21 cm Nd:PSMF placed in a F-P cavity formed by high reflector butt-coupled to coupling end of the fiber and Fresnel reflection of the other end facet. An output power of 1.42 W and a slope efficiency of 34.1% (18.4%) with respect to absorbed pump power (incident pump power) were obtained with 808 nm diode pumping. An increment as much as 9.7 and 15.0% in slope efficiency of the input coupling efficiency and the output power, respectively, were obtained by using a local-cooling design provided by watered sealing the coupling point. The repeatable results indicate that the design, featuring fluid sealing the coupling point of the fiber laser, which was capable of offering an effective alleviation of thermal effects and an elevation of the quality of the laser cavity, could be expected to be a convenient and effective scheme to improve the performance characteristics of the non-silica fiber lasers and the high power fiber lasers, generally in free-space coupling configuration.  相似文献   

16.
We demonstrate a cladding-pumped single-mode plane-polarized ytterbium-doped fiber laser generating 633 W of continuous-wave output power at 1.1 microm with 67% slope efficiency and a polarization extinction ratio better than 16 dB. The laser is end pumped through both fiber ends and shows no evidence of roll-over, even at the highest output power, which is limited only by the available pump power.  相似文献   

17.
An all fiber high power supercontinuum (SC) source is demonstrated by pumping a section of photonic crystal fiber (PCF) with a picosecond MOPA laser. The core of the PCF is enlarged at the input end through a serious of PCF post processing method to match the output fiber of the picosecond laser, to ensure low loss splicing, hence high power operation of the whole system. The supercontinuum output spectrum covers the wavelength range from 650 nm to beyond 1700 nm. Limited by available pump power, 20 W super-continuum output power is obtained under 29.5 W picosecond pump power, giving a high optical to optical conversion efficiency of 67.8%.  相似文献   

18.
从包层泵浦光纤激光器的速率方程理论出发,推导出了稳态下包层泵浦光纤激光器的输出功率,斜率效率和阈值功率的解析表达式,进行了数值模拟,对模拟结果进行了简单分析。并进行了实验研究,实验采用中心波长为975nm的激光二级管单端泵浦内包层形状为D型的包层光纤,利用二相色镜和光纤端面反馈构成谐振腔,采用了两套不同的准直耦合系统,得到的最高输出功率为24W,总的光-光转换效率为53.5%。  相似文献   

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