共查询到20条相似文献,搜索用时 140 毫秒
1.
2.
针对紫外-可见光谱水质检测系统单个LED光源输出功率低、光束质量差的问题,提出了一种多束紫外LED光源与光纤合束耦合的结构设计方案.运用ZEMAX光学分析软件开展了仿真设计研究,针对紫外LED光源与光纤耦合发散角较大的问题,设计了非球面准直透镜,准直后发散角为0.403 mrad;针对光束尺寸与光纤的匹配问题,进行了消色差双分离聚焦耦合透镜的设计.实验结果表明,合束LED光束汇聚的弥散斑的RMS尺寸为186.412 μm,GEO点尺寸为290.071 μm,光束中95%以上的能量集中在300μm以内,实现了多束LED光源与光纤的高效耦合. 相似文献
3.
基于单管半导体激光器光束传输特性,用光线追迹法对光纤耦合光路进行仿真分析,结果表明在激光器与光纤间放置圆柱透镜的间接耦合方法具有成本低廉、准直光束质量好等特性。根据光束传输几何关系,优化得到了准直距离L与圆柱透镜半径r比值为0.5时,准直效果最好,准直后发散角为2.45°。用光学仿真软件设计耦合光路,并对耦合光路进行光线追迹,结合产品的可靠性问题,最终得到优化的柱透镜直径为60μm。进行耦合实验,测量准直后发散角和采用水冷散热的耦合系统的耦合效率,准直后发散角约为2.55°,耦合效率最高为89.50%。耦合实验结果与仿真结果接近,满足了光纤激光器泵浦源的使用要求。 相似文献
4.
5.
6.
7.
为了压缩905nm的半导体激光,以用于远程测距,采用几何光路原理,设计了由两个相互垂直的椭圆柱面透镜组成的准直系统,并在ZEMAX软件的非序列模式下实现仿真。半导体激光器快慢轴的初始发散角为30°和15°,经过柱面透镜后,半导体激光器两个方向的发散角都大大压缩;经准直后,激光束的快慢轴发散角分别为4.4mrad和3.6mrad,基本满足了远程测距的要求。结果表明,椭圆面柱透镜对半导体激光有很好的准直作用。 相似文献
8.
9.
10.
11.
XUEChun-rong ZHUSheng-xiang XIAOZhi-gang 《半导体光子学与技术》2004,10(1):53-57,61
Transmission properties of tapered fiber including right cone fiber and bend optical fiber are discussed. The transmission efficiency of the tapered fiber is measured. The curve of transmission efficiency versus taper cone angle is given. By the scalar wave equation and Gaussian approximation, transmission properties of the two kinds of tapered fibers are analyzed, the power losses caused by taper cone angle and by the bending are also calculated. From the experiments and theoretical analysis, it could come to a conclusion that the wider the taper cone angle is,the higher the transmission efficiency will be. 相似文献
12.
13.
倏逝波的透射深度、均匀感应区域的感应芯径和感应长度是线性锥形光纤倏逝波传感器灵敏度的主要影响因素。为了实现灵敏度的最优化设计,分别建立了倏逝波透射深度与锥形参数之间关系及有效吸收路径与感应芯径和感应长度之间关系的数学模型,讨论了不同锥形参数(发射角、锥度比、锥长)下倏逝波的透射深度,不同感应芯径和感应长度下倏逝波的有效吸收路径,并进行了仿真。仿真结果表明,选择锥形光纤几何体和合适的发射角,可使透射深度增大近3倍,当锥度比为0.4时,倏逝波透射深度最大;减小感应芯径,增大感应长度可提高倏逝波的有效吸收路径,增强纤芯表面的倏逝波与周围吸收介质的作用强度。研究结果可用来指导制作高灵敏度线性锥形光纤倏逝波传感器。 相似文献
14.
Golden J.P. Anderson G.P. Rabbany S.Y. Ligler F.S. 《IEEE transactions on bio-medical engineering》1994,41(6):585-591
For pt.I see ibid., vol.41, no.6, p.578-84 (1994). A biosensor was developed using antibodies, fluorescence and the evanescent wave to detect antigen binding at the surface of an optical fiber. Cladding was removed from the core along the distal end of a step-index optical fiber, and recognition antibodies were immobilized on the declad core to form the probe sensing region. Immersing the declad probe in aqueous solution creates a V-number mismatch between the immersed probe and the clad fiber. Probes created with reduced sensing region radius exhibited improved response by decreasing the V-number mismatch. Tapering the radius of this region has further improved probe response. Ray tracing analysis of the tapered probe demonstrated that the evanescent wave penetration depth increases along the length of the taper. Experiments correlating position of refraction along the taper with launch angle at the proximal end were realized in the ray tracing model. An evanescent wave immunoassay was performed with a series of the tapered fiber probes, each tapered from the fiber core radius (100 μm) to different end radii. An end radius of 29 μm was found to produce maximal signal from the tapered probe. Factors leading to the determination of the optimized probe are discussed 相似文献
15.
锥形光纤的功率分布特性 总被引:2,自引:1,他引:2
从波动理论出发,对锥形光纤的纵向传播常数进行泰勒(Taylor)级数展开,经近似得到了锥形光纤功率分布的解。基于此理论,对锥形光纤的功率分布特性进行了讨论,并分析了锥形光纤的长度、锥度和光纤折射率等参数对锥形光纤不同模式功率分布的影响。为了减小功率泄漏,当光从锥形光纤大端入射时,应当减小锥长,减小锥度,增大纤芯包层折射率差;当光从锥形光纤小端入射时,应当增加锥长,增加锥度,增大纤芯包层折射率差。在长锥长、大锥度情况下,光纤折射率分布的影响相对较小。 相似文献
16.
锥形光纤的结构与特性 总被引:1,自引:0,他引:1
通过理论分析和仿真试验,研究了锥形光纤的几何形状对锥形光纤的传输损耗和耦合效率的影响.用几何光学的分析方法,说明了光信号在锥形光纤中的传输损耗远低于同类型的圆柱形光纤;仿真试验研究了光源与光纤的相对位置、锥形光纤的尖端半径、锥形光纤的锥角大小对锥形光纤耦合效率的影响. 相似文献
17.
锥度光纤作为相位共轭镜具有高反射率、高保真度等优点,将3根自制的、规格不同的锥度光纤相位共轭镜应用在重复频率100Hz,脉宽28ns的激光二极管(LD)抽运的高功率脉冲激光主振荡功率放大器(MOPA)系统中,对其受激布里渊散射(SBS)性能以及锥度区尺寸的影响进行了研究。结果表明,芯径大于400μm的大尺寸锥度光纤可以应用于高功率激光系统中,如选择较长的后端光纤长度以及适当的锥度区规格可获得较高的受激布里渊散射能量反射率和输出能量。在应用总长5.2m,锥度区从φ400μm过渡到φ200μm的锥度光纤时,实验获得了高达85%的受激布里渊散射能量反射率和大于21mJ的双通输出能量,激光脉宽被压缩到17ns,最大峰值功率达到兆瓦量级。 相似文献
18.
The authors consider a tapered velocity coupler (TVC) that meets the adiabatic invariance condition with sufficiently strong coupling between the fundamental modes of individual guides in the middle region of the coupler while permitting individual excitation at the input end and sorting of the modes at the output end. This approach helps reduce the device length considerably by permitting much higher taper angle. A TVC consisting of one tapered and another straight, graded index waveguide is modeled using the normal modes of the entire, composite TVC structure. The analytical results are in excellent agreement with experimental results for a TVC fabricated in Ti:LiNbO3. It is shown that the representation of the local normal modes as the superposition of the modes of the uncoupled guides leads to erroneous results 相似文献
19.
20.
The novel waveguide structures described in this paper have nonlinearly tapered shapes that result in low radiation losses despite their relatively short lengths. The core at the waveguide endface connected with the fiber has a very small cross section and an expanded mode field with a non-Gaussian shape. The taper structures are analyzed by using an improved step-transition method. This method is a based on the theory of enclosing a waveguide within electrical walls and that can therefore treat the radiation modes in a tapered waveguide as discrete mode spectra. Analyzing the relationships between the lengths and shapes of the tapers and the radiation loss due to the tapers show that appropriately tapered semiconductor waveguides operating at an optical wavelength of 1.55 μm and having a taper length of less than 0.7 mm can have a radiation loss of only 0.1 dB and a coupling loss with a conventional single-mode fiber of less than 0.5 dB 相似文献