CO2激光加热硅芯光纤预制棒的温场分布

研究了10.6 m CO2激光加热硅芯光纤预制棒的温场分布，在考虑预制棒表面热辐射和空气对流的情况下，用有限元软件COMSOL Multiphysics建立了激光加热预制棒的传热物理模型，比较了激光功率、激光光斑半径和预制棒直径对温场分布的影响，同时提出CO2激光加热与石墨炉加热结合调节温场分布的方法。仿真结果显示，激光参数和预制棒直径都会明显影响预制棒温场分布，且激光光斑半径3 mm，功率达到400 W的激光器可用于直径10 mm内的硅芯光纤预制棒制备硅芯光纤。通过CO2激光加热和石墨炉加热相结合的加热方式，能更加灵活有效地调节预制棒的温场分布，构建适合硅芯光纤拉丝的温场条件。     

基于平行平板的折射率高精度非接触测量

常用的测量折射率的方法如偏向角法、自准直法、临界角法、 V棱镜法等,这些方法通常需特制三棱镜与待测件。待测样品不一致且过程复杂,测试定标周期长,难于自动化。为了保证待测材料的完整及实现自动化测量,进行了基于平行平板的折射率非接触测量的尝试。运用该方法进行折射率的测量,不需特制三棱镜并且待测件与待测样品一致。分析表明,通过选择合适的测量角度,该方法旋转角度精度为a=0.003（即10）,导轨精度为L=0.000 8 mm,平行平板厚度测量精度为d=0.001 mm。     

传像光纤、光纤面板及光锥制造新方法探索

利用高折射率光纤填充微结构预制棒孔洞的方法,制造直径70 mm、长度200 mm的大尺寸传像光纤预制棒,像素数为547.为提高传像元件的像素数,将预制棒先拉伸成直径约为30 mm的二次预制棒,通过切削、并熔后拉伸,得到像素数为3829的传像微结构光纤及其面板和光锥,其理论数值孔径为0.55.经初步测试发现,其传像效果良好.此方法利用微结构光纤技术制造传像光纤、面板和光锥,简单易行,成本低,能有效提高像素数,有望成为规模化制造高分辨率、高质量传像元件的新方法.     

传像光纤、光纤面板及光锥制造新方法探索

利用高折射率光纤填充微结构预制棒孔洞的方法,制造直径70 mm、长度200 mm的大尺寸传像光纤预制棒,像素数为547.为提高传像元件的像素数,将预制棒先拉伸成直径约为30 mm的二次预制棒,通过切削、并熔后拉伸,得到像素数为3829的传像微结构光纤及其面板和光锥,其理论数值孔径为0.55.经初步测试发现,其传像效果良好.此方法利用微结构光纤技术制造传像光纤、面板和光锥,简单易行,成本低,能有效提高像素数,有望成为规模化制造高分辨率、高质量传像元件的新方法.     

聚焦法测量梯度折射率透镜的折射率分布

本文针对梯度折射率分布的透镜(以后简称梯析透镜)与光纤在折射率分布上的不同点,对用于光纤及其预制棒测量的聚焦法的原理公式,计算测量方法等进行了重要改进,从而使聚焦法可适用于梯折透镜的测量.本文通过计算机模拟计算,对原理公式及计算方法的准确性和可靠性进行了验证,并同时给出了这一测量方法的精度,最后给出了测量实例及其比较结果.     

离子交换引起的GRIN棒透镜大折射率差值分析

利用两次离子交换法制作了GRIN棒透镜样品，并采用雅明干涉法对样品的折射率分布进行了测试.结果表明，样品获得了较大的折射率差值.讨论了两次离子交换增大折射率差的原因.研究结果在制作生产梯度折射率材料方面有一定的参考价值和指导意义.     

微结构光纤预制棒拉制过程的温度场分布

根据非稳态傅里叶热传导方程及微结构光纤(MSF)预制棒的初始条件和边界条件，建立圆柱形坐标系，推导出MSF预制棒的温度场分布方程.计算结果表明：当MSF预制棒在高温炉内的温度场分布接近热传导稳态分布时的下棒速度为制备MSF的最佳速度，此时高温炉的加热温度可降低到MSF预制棒的软化温度，另外，随着MSF空气填充率的增加，MSF预制棒的下棒速度也应加快. 关键词： 微结构光纤 光纤预制棒 温度场分布 热传导     

低色差GRIN棒透镜制备工艺的研究

熔制了含Li+硅酸盐玻璃,玻璃的棒料在NaNO3熔盐中进行离子交换后得到了梯度折射率(GRIN)棒。采用干涉法测得了GRIN棒的折射率分布曲线。实验结果表明:通过所述的工艺,可以获得直径达5mm的GRIN棒,其折射率分布曲线与双曲正割曲线接近。分析表明GRIN棒的轴向色差评价函数值约为0 6～0 7%。     

用毛细管焦点法精确测量微量液体的折射率

介绍了用毛细管焦点法精确测最微量液体折射率的一种新技术.该技术基于共轴球面光学系统的成像原理,用LED(λ=580 nm,FWHM为32nm)为测量光源,用CCD为像接收装置.一次测量样品需要量小于0.002 mL.待测样品封闭在毛细管内测量,有利于对毒性、挥发性和吸湿性强的液体介质折射率的测量.用此技术对纯水、乙醇、乙二醇和丙三醇样品的折射率做了测量,测量精度分别为0.0001,0.0002,0.0003和0.0003.论文在分析实验装置的测量灵敏度和成像景深基础上,提出了进一步提高测最精度的方法.     

用光束偏折法测光纤预制棒的折射率分布

<正> 折射率的分布是光纤的重要测量参数之一,其测量的方法甚多。近年来,对于光纤的折射率分布的非破坏性测量已进行了不少工作。本文采用“光束偏折法”进行非破坏性测量,共分二部分。第一部分是测定预制棒包皮的折射率值,第二部分是对没有包皮的预制棒     

Nondestructive index profile measurement of noncircular optical fibre preforms

We present quantitative results for the effect of noncircularity on a method recently proposed by Chu for the measurement of the refractive index profile of an optical fibre preform. Analytical studies show how Chu's method can be applied to elliptical preforms.     

Determination of the refractive index profile of polymer optical fiber preform by the transverse ray tracing method

In graded-index polymer optical fiber (GI-POF), the refractive index profile is an important parameter in defining its bandwidth. However, direct determination of the refractive index profile of GI-POF is difficult due to its extreme thinness. In this study, the refractive index distribution of the GI-POF is indirectly determined by measuring the refractive index distribution of the GI-POF perform by applying the transverse ray tracing method to a simplified measurement system that we developed.In this system, a parallel tabular ray is irradiated transversely to a GI-POF preform. The transverse ray from the preform is then projected on a screen, and its digital image is processed to calculate the refractive index distribution. The calculation is based on a transverse ray simulation, a computer program that we developed in which the refractive index distribution of the preform is determined by comparing the displacement of the transverse ray projected on the screen with the actual measurement.The accuracy of this new measurement method is validated by comparing the refractive index distribution of a GI-POF preform with the refractive index distribution measured by the conventional method using an interferometer. We find that the refractive index distribution measured by this novel method agrees well with that measured by the conventional method.     

Determination of the refractive index profile of a symmetric fiber preform by the transport of intensity equation

The refractive index profile of an axially symmetric fiber preform is determined by using the transport of intensity equation. In this method the preform is immersed in an index-matching liquid, and a collimated light beam impinges on it laterally. The intensity distributions of the transmitted light are measured on two close parallel planes inside the preform core. From the recorded intensity distributions, the deflection function is calculated by the transport of intensity equation. The refractive index profile is obtained by means of Abel inversion. Also, for comparison, the refractive index profile of the preform is measured by the focusing method and the results are in agreement with less than 3% error.     

Axial refractive index depression in preforms and fibers

The refractive index depression that exists along the axis in modified chemical vapor deposited (MCVD) preforms and fibers doped mainly with GeO₂ or P₂O₅ is studied by interference microscopy. The index profile of a preform, determined as a function of its transition from the uncollapsed to the fully collapsed state, shows that this central region is fully depleted of dopant and has an index value corresponding to that of the pure fused silica cladding. The same results are found in samples taken from six preform tips and from a relatively large fiber, indicating that this effect is a general property of an uncompensated fabrication process. Implications for its influence on the fiber's transmission properties are discussed.     

Fluorescence characterization and gain studies on a dye-doped graded index polymer optical-fiber preform

Preparation of an appropriate optical-fiber preform is vital for the fabrication of graded-index polymer optical fibers (GIPOF), which are considered to be a good choice for providing inexpensive high bandwidth data links, for local area networks and telecommunication applications. Recent development of the interfacial gel polymerization technique has caused a dramatic reduction in the total attenuation in GIPOF, and this is one of the potential methods to prepare fiber preforms for the fabrication of dye-doped polymer-fiber amplifiers. In this paper, the preparation of a dye-doped graded-index poly(methyl methacrylate) (PMMA) rod by the interfacial gel polymerization method using a PMMA tube is reported. An organic compound of high-refractive index, viz., diphenyl phthalate (DPP), was used to obtain a graded-index distribution, and Rhodamine B (Rh B), was used to dope the PMMA rod. The refractive index profile of the rod was measured using an interferometric technique and the index exponent was estimated. The single pass gain of the rod was measured at a pump wavelength of 532 nm. The extent of doping of the Rh B in the preform was studied by axially exciting a thin slice of the rod with white light and measuring the spatial variation of the fluorescence intensity across the sample.     

人工水晶钻石白度的检测方法

利用阿贝折射仪检测了人工水晶钻石的折射率，介绍了以不同固体的折射率为标准进行人工水晶钻石的白度分析的方法．     

表面等离激元探针的高介电灵敏度与液体折射率测定

利用金纳米棒在光照射下激发表面等离激元的性质,实验研究了其在不同介电环境下的吸收光谱.通过分析纵向等离子体共振吸收峰峰位随介质折射率的变化,获得了金纳米棒表面等离激元探针测量介质折射率的经验公式为n=(385.59)-1(λ/nm-290.56).利用金纳米棒表面等离激元探针的高介电灵敏度,测试了一些未知液体的折射率,并与阿贝折射仪测量法的结果相比较.结果与分析表明,本方法较之阿贝折射仪测量介质折射率的方法具有更高的精密度.因此,表面等离探针可用于拓展大学物理实验中的介质折射率测量实验.     

Refractive index dispersion measurement on nonlinear optical polymer using V-prism refractometer

By using V-prism refractometer, the refractive indices of a polyetherketone (PEK-c) guest–host polymer system were measured with the polymer in solutions. The Lorenz–Lorentz local field formalism was used in the calculation of the refractive indices of the polymers from the measured indices of the polymer solutions and the pure solvent by using V-prism refractometer. The refractive index dispersions of the polymers were obtained by fitting the measured indices of the polymers to Sellmeyer equation. The method allows for an accuracy in index of 0.7% in the determination of the polymer indices. In addition, a large difference between the indices of the polymer and the solvent, and a higher polymer volume fraction in the measured polymer solution are favorable for a high accuracy.