普通单模石英光纤中频率上转换过程的研究

介绍了在普通通讯用单模ＧｅＯ２／ＳｉＯ２石英光纤中从近红外到可见光的频率上转换过程。利用１．３１３μｍ的调Ｑ锁模Ｎｄ：ＹＬＦ激光脉冲泵浦单模石英光纤，产生了５８８ｎｍ的黄光，峰值功率达２０Ｗ，对应０．０９％的转换效率。     

用改进的分光计测量光纤理论数值孔径

为测量光纤数值孔径,对分光计进行改动,将准直管和望远镜系统对调,使准直管可以绕中心轴转动,采用体积小亮度高的LED作光源,并将其固定在准直管进光孔的狭缝处,以产生可以转动的平行光. 用改进后的分光计测量光纤的数值孔径,取得了满意的结果. 该方法简单易行,特别适用于大学层次的物理实验.     

大数值孔径多组分玻璃柔性光纤的制备及影响因素分析

大数值孔径多组分玻璃柔性光纤在医用光纤内窥镜中具有广阔的应用前景.采用La2O3 -Nb2O5 -SiO2-B2O3-RO玻璃系统作纤芯,用自制相匹配的低折射率玻璃材料作包层拉制的柔性光纤的数值孔径为0.8725,光的接受角为122°,扩大了医用光纤内窥镜的观察范围,满足了医疗仪器观察诊断的特殊需要.给出了La2O3 ...     

单模石英光纤中连续波泵浦SRS谱的演化

利用连续波掺Yb双包层光纤激光器为泵浦源,对单模石英光纤中受激Raman散射谱的形成过程进行了实验研究结果表明,由自发Raman散射向受激Raman散射演化的过程中Stokes谱宽度不断变窄当Stokes波信号功率较强时,在Raman光谱内部会出现能量红移现象,使Stokes光谱峰值相对于泵浦波的频移量从440cm^-1转化到490cm^-1.     

环状光纤单模条件和远场能量分布特性

基于弱波导近似,通过数值计算得出了环状光纤保持单模状态时对芯-包层折射率差值和导光层厚度的要求,同时讨论了这些设计参数对远场能量分布的影响。计算结果表明:当环状光纤工作在单模状态时,从光纤出射的环形光束衍射至远场时形成一个中央亮斑,具有很高的能量集中度。此外,减小芯-包层折射率差值与导光层厚度有利于进一步减小远场衍射的光斑宽度。     

环状光纤单模条件和远场能量分布特性

基于弱波导近似,通过数值计算得出了环状光纤保持单模状态时对芯-包层折射率差值和导光层厚度的要求,同时讨论了这些设计参数对远场能量分布的影响。计算结果表明:当环状光纤工作在单模状态时,从光纤出射的环形光束衍射至远场时形成一个中央亮斑,具有很高的能量集中度。此外,减小芯-包层折射率差值与导光层厚度有利于进一步减小远场衍射的光斑宽度。     

温度变化对单模石英光纤受激拉曼散射附加峰的影响

用10 m长单模石英光纤进行受激拉曼散射温度特性研究, 实验中发现在泵浦光和一级Stokes左右出现了附加峰(称为双峰), 其峰强度随温度的升高(80～295 K)呈现先增加后减弱现象。当温度达到295 K时, 一级Stokes双峰消失。由受激四光子混频理论计算可知,这种双峰现象是受激四光子混频的结果。同时对SRS一级Stokes所产生的受激四光子混频的Stokes频移随温度升高由706.9 cm-1增大到712.9 cm-1和其半宽度由1.75 nm增至2.18 nm的现象也进行了解释。     

测量单模光纤模场直径的一种新方法

本文根据单模光纤模场直径的横向位移定义,提出了一种测量模场直径的新方法——远场高斯掩模匹配法.讨论了几种测量及数据处理方法.最后给出了初步的实验结果.     

光纤数值孔径与衰减系数的测量实验

基于光纤数值孔径与衰减系数的概念和测量原理,搭建了相应的实验测量系统,实际测量了光纤的数值孔径和衰减系数,并对实验结果进行了分析。     

宽温低损耗单模光纤定向耦合器

本文报道了用熔融法由常规的单模通信光纤制造宽温工作的低损耗单模光纤定向耦合器.工作波长为1.52μm,分束比为50%的封装器件;工作温度在-30～+70℃范围,分束比容差小于±5%,插入损耗<0.2dB,隔离度>40dB.工作波长的变化对分束比影响十分明显,但入射光的偏振态对其无实际影响.     

单模石英光纤弯曲损耗的测量——光纤弯曲损耗特性的设计性实验

阐述了利用布拉格光纤光栅传感器测量单模石英光纤弯曲损耗实验的原理、方法和步骤.该实验是一个关于光信号在光纤中传输时由于弯曲而产生损耗的设计性实验,既能丰富实验教学内容,又能开拓学生的视野,提高学生的创新能力.     

Status of single-model optical fiber standardization in the electronic industries association (EIA)

This paper introduces and analyzes revolutionary laser system architecture capable of dramatically reducing the complexity of laser systems while simultaneously increasing capability. The architecture includes three major subsystems. The first is a phased array of laser sources. In this article, we discuss diode-pumped fiber lasers as the elements of the phased array, although other waveguide lasers can also be considered. The second provides wavefront control and electronics beam steering, as described in an IEEE Proceedings article on “Optical Phased Array Technology” [1]. The third is subaperture receiver technology. Combining these three technologies into a new laser systems architecture results in a system that has graceful degradation, can steer to as wide an angle as individual optical phased array subapertures, and can be scaled to high power and large apertures through phasing of a number of subapertures. Diode-pumped fiber lasers are appealing as laser sources because they are electrically pumped, efficient, relatively simple, and scalable to significant power levels (over 100 Watts has been demonstrated from a single diode-pumped fiber laser) [2]. The fiber laser design also lends itself to integration into a phased array. Fiber lasers have been phased. Initial phasing demonstrations have been at low power and were conducted by taking a single source, dividing it into multiple fibers, then phasing them together. To develop this technology further we need to use independent fiber lasers or fiber amplifiers, seeded by a common source, and to increase laser power. As we increase laser power, we will have to learn to cope with nonlinearities in the laser amplifiers. Optical Phased Array technology has demonstrated steering over a 90-degree field of regard [4], although this approach used additional optical components. If we use straightforward optical phased array beam steering without additional optics we can steer with high efficiency to about one-third λ/d, where d is the smallest individually addressable element. The one-third factor depends on the efficiency threshold. For example, if we use 1.5 μm light, and 5 μm center-to-center spacing, we can steer with high efficiency to about ±6 degrees, or a field of regard of 12 degrees. Last, we need to develop a subaperture receive technology. This can be a pupil plane receiver, an image plane receiver, or some combination of the approaches. When we have matured each individual technology and combined them into new laser systems architectures, we will have the ability to build simpler and more capable laser systems. The vision for an integrated, phased array laser concept is to enable a new class of laser systems with significant advantages, including high-efficiency, all-electric laser source; all waveguide beam transport; wavefront control at the sub-aperture level (enabling wavefront compensation, conformal apertures, and wide-angle electronic beam steering); random access beam pointing over wide angles; multiple simultaneous beam generation and control; and graceful degradation.     

石英光纤的金属镍锡涂敷工艺研究

为了实现石英光纤传感器的无胶金属化封装,需要在光纤表面涂敷金属层。先利用化学镀方法在石英光纤表面镀镍层,再利用电镀工艺电镀锡层,从而获得表面光亮、均匀、附着牢固、可焊性好的金属涂敷层。实验中研究了敏化、活化工艺对镀层的影响并提出一种效果较好的敏化活化方法。给出了石英光纤表面化学镀镍的最佳工艺条件。     

锥台光纤的功率转换效率研究

 锥台光纤在激光束到单模光纤以及多模光纤到单模光纤的耦合中,在一些需要质量很高光束的同时有较高功率要求的场合有广泛应用。在这些应用中,锥台光纤的功率转换效率是很重要的一个参数。介绍了锥台光纤的熔拉研磨制作方法,分析了锥台光纤的传输特性。建立了高斯近似模型,采用模场耦合理论,计算了锥台光纤的功率转换效率。在以下参数条件下对细端半径分别为（4±1）μm,(5±1)μm,(6±1)μm,(7±1)μm和(8±1)μm的锥台光纤的功率转换效率进行了实验测定,激光器输出光波长532 nm;多模光纤NA＝0.11,纤芯半径a=12.5 μm;得到了与理论计算吻合的结果。     

基于包层模谐振的三包层石英特种光纤温度传感特性研究

提出了一种基于包层模谐振的光纤温度传感器. 它是通过将三包层石英特种光纤(TCQSF)两端分别与普通单模光纤(SMF)电弧熔接构成的SMF-TCQSF-SMF结构. 根据耦合模理论, 首先将TCQSF等效为三个同轴波导, 按各波导模场的分布特点标量计算其传输模式的色散曲线, 并深入研究其耦合长度与传输谱线之间的关系; 其次根据光纤的热光效应及热膨胀效应, 分析计算该传感器的温度灵敏度; 最后选取耦合长度为一个拍长时的传感器进行温度传感实验. 实验结果表明, 在35-95 ℃的温度变化范围内, 其温度灵敏度为73.74 pm/℃, 与理论计算结果一致. 因此, 该传感器具有结构简单、制备容易、灵敏度高、包层模激发可控等优点, 可用于工业生产、生物医学等温度传感领域.     

Fiber optic evanescent field absorption sensor: Effect of fiber parameters and geometry of the probe

A comparative experimental study of the fiber-optic evanescent field absorption sensor based on straight and U-shaped probes is presented. The effects of numerical aperture and the core radius of the fiber on the sensitivity of the sensor are experimentally investigated. Increase in the numerical aperture of the fiber increases the sensitivity of the sensor in the case of both the probes. The effect of core radius on the sensitivity depends on the bending radius of the probe. In the case of straight probe (i.e. infinite bending radius) the fiber with smaller core radius has high sensitivity while in the case of U-shaped probe with 0.17 cm bending radius, the fiber with larger core radius has high sensitivity. Thus, which fiber (with small or large core radius) has maximum sensitivity depends on the bending radius of the probe. For a given fiber, decrease in the bending radius increases the sensitivity of the U-shaped probe. An inverse power law relationship between the bending radius and the evanescent absorbance and hence the sensitivity is established.     

光纤端面反射对高功率光纤放大器特性的影响

 从光纤端面研抛工艺的技术特点出发,计算了端面倾角和反射率的关系,估算了斜面研抛后端面反射率的大小。在掺Yb³⁺双包层光纤放大器理论模型的基础上,数值模拟了常规研抛角度误差造成的端面反射率对放大器输出特性的影响。计算结果表明：端面反射导致系统内出现严重放大的自发辐射和自激现象,减小光纤两个端面的反射率是最有效的抑制方法,同时,增大入射信号激光功率也可以抑制自激,提高输出信号光功率和信噪比。     

干涉测距仪中光纤的特性分析

提出一种由定位干涉仪和测量干涉仪组成的光纤干涉绝对距离测量方法 ,将对光程的定位过程和对距离的测量过程分别进行 ,实现对大距离的高精度绝对测量 ,同时在测量系统中引入光纤和光纤干涉仪 ,以改善系统结构和性能。详细分析了光纤损耗特性、色散特性和偏振特性对测量系统的影响 ,并特别给出了有关色散特性影响的量化分析结果。分析表明色散特性对于系统的测量范围有较大的影响     

石英音叉陀螺音叉封装问题研究

封装是石英音叉陀螺的关键工艺,封装管壳的选择、封装方式及石英音叉的固定形式对音叉的性能有直接影响。封装管壳的有限元仿真分析,可以作为封装管壳选取的依据。采用单点固定封装方式有利于石英音叉工作性能的稳定。实验中通过改变封装盖板的开合状态来改变封装方式,石英音叉的阻尼和品质因数发生了明显的改变。