塑料光纤双锥与半球腔的活动耦合效应

报道了用氮氖激光实现的塑料光纤双锥与介质半球(称半球腔)之间的活动耦合效应。测量了光纤双锥的发射效率，并测量了锥腔耦合效率与半球腔的表面积、锥腔距离之间的关系。根据这种效应，可以制成塑料光纤活动耦合器；如果再加上调谐滤波器，可制成适合塑料光纤通信网用的信号上下载装置。     

四端口光纤声光器件的耦合模理论

简述了光纤的声致折变机制,在复合光波导理论基础上讨论了光纤零耦合器与常规光纤耦合器的本质区别,指出零耦合器实质上是一段可以选择激励的双模光纤。从耦合模理论出发,求解了零耦合器中声致模耦合渐进方程组,给出了四端口光纤声光器件功率耦合的完整解析表达式,阐明了器件输出光的频移特性,解释了器件在声光谐振时具有的倍频声光调制、可调光移频、光滤波、光分束、光开关等功能。最后报道了器件作为可调光分束器或光开关的研究实例。     

双锥型光纤布喇格光栅光谱特性

利用传输矩阵法和有限元法分析了光栅周期、调制深度、锥腰直径和不同设计区段长度比等光栅制作参量和结构设计参量对双锥型光纤布喇格光栅光谱特性的影响.软件仿真结果表明:限定相关参量后,光栅周期增大,双锥型光纤布喇格光栅整体反射谱右移,与均匀分布光纤布喇格光栅光谱变化规律一致;调制深度增强,两主反射峰基本不变,而两主反射峰中间的次级峰个数增多,光强增大;锥腰直径减小,激发更多包层模,干涉峰个数增多,强度提升;整根光栅长度保持1cm不变,锥腰区,标准光栅区和渐变光栅区长度比直接影响次级峰的数量和幅值,随着渐变光栅区长度占比的增大,次级峰的幅值增大,同时个数减少.双锥型光纤布喇格光栅可在多参量传感器、多通道滤波器、多通道半导体激光器、色散补偿和光上下载分插复用等方面广泛应用.     

双锥光纤模拟理论方法

从双锥光纤的工艺实现和技术应用目的出发,建立了可与实验上易测量的工艺参数相联系的高期型等效双锥光纤模拟理论方法,可用于双锥光纤的制作及光学特性的分析,数值模拟结果与实验符合得很好。     

超高速光纤耦合声光调制器的设计及其应用

为实现小于10 ns光脉冲上升时间的超高速声光调制,该文提出一种光纤耦合声光调制器光脉冲时域响应的理论设计仿真方法。利用该方法对1064 nm和1550 nm工作波长光纤耦合声光调制器进行了仿真,结果预测器件的光脉冲上升时间分别为9.4 ns和9.1 ns;通过器件制作和测试验证,两个波长的器件实测光脉冲上升时间分别为9.74 ns和9.22 ns,实测与理论仿真结果偏差较小。文章最后对器件在超快光纤激光器种子源光脉冲选单、光纤水听阵列时分复用及潜在的宽带移频应用进行了介绍。     

全光纤声光调制器的耦合模理论研究

利用适于普通通信光纤的耦合模方程,从理论上分析了一种全光纤声光调制器.并从理论上研究了基于普通通信光纤的全光纤声光调制器,得到了这种全光纤调制器的输出结果.     

基于光纤叠栅的全光纤声光可调谐滤波器的特性分析

本文提出了一种基于光纤叠栅的全光纤声光可调谐滤波器, 与普通光纤布拉格光栅型全光纤声光可调谐滤波器相比, 该滤波器能够对光纤叠栅的两个中心波长进行同步调制. 理论分析了声波频率和声致应变幅度对基于光纤叠栅的全光纤声光可调谐滤波器的传输光谱的影响, 结果表明, 各阶次反射峰分别以两个主反射峰为中心呈对称关系, 且主反射峰与其所调制出的次反射峰之间的波长间隔与声波频率成正比, 而两个主反射峰所调制出的同阶次反射峰之间的波长间隔与声波频率无关; 声致应变幅度主要影响主反射峰及次反射峰的反射率的变化. 实验中, 分别测试声波频率为390 kHz和710 kHz的基于光纤叠栅的全光纤声光可调谐滤波器的传输光谱, 实验结果的变化趋势与仿真分析结果相一致.     

基于石英柱模型的光子晶体光纤异常布里渊散射特性的理论研究

通过石英圆柱模型,理论研究了小芯径光子晶体光纤中混合声波模式的色散、模式耦合以及声光相互作用,理论计算出了布里渊散射增益系数谱的双峰结构及其随抽运光波长和温度的演化规律. 理论分析表明光子晶体光纤中布里渊散射增益系数谱的双峰结构源于小芯径光子晶体光纤中混合声波模式之间的模式耦合. 通过温度改变导致的材料参数变化对声波模式色散特性的影响,特别是声波模式耦合点的移动,解释了双峰结构随外界温度的变化规律. 并且,通过理论计算与实验结果的对比讨论了石英圆柱模型的局限性和适用范围. 关键词： 布里渊散射 声光相互作用 模式耦合 光子晶体光纤     

熔锥型熊猫光纤耦合器的传输特性分析

熔锥型保偏耦合器的传输特性决定了其光学原理与功能的实现。为了从理论上分析各参量对保偏耦合器传输特性的影响,基于热-结构-电磁多物理场耦合理论,建立了熔锥型熊猫光纤耦合器双锥模型,应用有限元法,分析了各参量对熊猫光纤耦合器传输特性的影响。结果表明应力区与包层折射率差影响耦合区纵向电磁场的分布,折射率差越大,纵向电磁场分布的变形也越大;HE1x1模和HEy11模的传播常量对偏振主轴角度差不敏感,偏振主轴角度差是通过耦合系数进而影响保偏光纤耦合器的消光比的;HE1x1模的传播常量对熔锥的熔锥区横截面椭圆率比较敏感,横截面椭圆率变化6.67%时Δβx11变化0.14%,计算结果表明当熔锥区横截面椭圆率为0.56时可获得较高性能的耦合器。     

环形腔声光可调谐掺铒光纤激光器调谐范围的研究

介绍了一种基于声光可调谐滤波器(AOTF)的可调谐掺铒光纤激光器。从掺铒光纤放大器的速率方程和传输方程出发,推导出声光可调谐掺铒光纤激光器的输出公式,理论上解释了该环形腔声光可调谐掺铒光纤激光器调谐范围仅决定于掺铒光纤的增益带宽;并在实验中测得该激光器调谐范围为1 526.05 nm到1 560.63 nm,这个区间对应着实验所得掺铒光纤自发辐射谱的增益区间,从而验证了理论推导所得结论。     

利用声光衍射测量海水中悬浮沙浓度的研究

本文提出了利用声光衍射来测量海水中悬浮沙浓度的方法.依据声光衍射理论和超声在悬浮液中传播特性,推导出声光衍射损耗系数之比与悬浮沙浓度的关系式,并利用He-Ne激光器,对浓度低于1kg/m³的高岭土海水悬浮液进行了实验.     

声光可调谐滤光器的光谱传递特性和数据恢复方法

本文在分析声光可调谐滤光器透过特性的基础上。对其引入了光谱传递函数的概念,并计算和讨论了光谱传递函数随滤光器结构参数的变化规律。     

声光效应实验研究

介绍声光效应的最新理论进展。采用光栅假设，对各向同性介质中的声光效应作了简要讨论，导出了第m级衍射光的衍射效率公式。研究和介绍一种新的声光效应实验装置。在实验中，应用线阵CCD光强分布测量仪等，通过改变超声波的频率和功率，分别实现了对激光束方向的控制和强度的调制；定量给出了声光偏转量的关系曲线和声光调制测量的关系曲线。实验表明，在布喇格衍射下，通过固定超声波功率，测量衍射光相对于零级衍射光的相对光强与超声波频率的关系曲线，不仅可以计算声速，还可以确定声光器件的带宽和中心频率。     

On the possibility of extending the dynamic range in acoustooptic analysis of the spectrum of radio signals

A method is proposed to suppress nonlinear distortions arising in the acoustooptic analysis of the spectrum of radio signals. The method is based on the polynomial nonlinear correction of an electric signal before it comes to a piezoelectric transducer. The necessary form of the correction is determined in a wide range of parameters of the acoustooptic interaction. The results of numerical simulation are presented.     

Optimization of the characteristics of an acoustooptic cell based on a tellurium crystal

The problem of designing acoustooptic devices based on tellurium crystals intended for operation in the wavelength range λ > 5 μm is discussed. The optimum geometry of the isotropic acoustooptic interaction in this material is found. The problem of searching for the optimum geometry of a filter that uses anisotropic-acoustooptic interaction is analyzed.     

Acoustooptic multiplication of the frequency shift of optical radiation on the basis of bragg polarization splitting

A technique for the acoustooptic multiplication of the frequency shift of an optical beam is proposed. The technique is based on the cascade diffraction of the beam by a single acoustic wave with the use of Bragg polarization splitting in a uniaxial crystal. The fundamental possibility of the practical realization of the technique is confirmed experimentally by using anisotropic acoustooptic diffraction in LiNbO₃.     

Light diffraction on ultrasonic Love waves

It is shown that layers based on acoustooptic crystals excited by ultrasonic Love waves can be used as light modulators in the reflection and transmission mode. It is established that various modes of Love waves can be detected by optical methods. For small ultrasound intensities, the diffraction efficiency is determined by the degree of homogeneity of deformations within the layer, and for large intensities, by the length of the acoustooptic interaction.     

Investigation into the acoustooptic properties of tellurium crystals by anisotropic diffraction of light

The optical, acoustic, and acoustooptic properties of tellurium crystals viewed as a candidate material for mid-and far-IR acoustooptic devices are considered. The phase velocities, polarization, and drift angles of the acoustic energy in different crystal planes are calculated. The acoustooptic figure of merit for tellurium under the anisotropic diffraction conditions is estimated, and light-sound interaction geometries promising for acoustooptic applications are discussed. Measuring data for the optical and acoustooptic parameters of tellurium crystals are given.     

Acoustooptic nonpolar light controlling devices and polarization modulators based on paratellurite crystals

A complex of investigations and projects aimed at solving problems of highly effective acoustooptic control of nonpolarized laser radiation is generalized on the basis of anisotropic Bragg’s diffraction in a TeO₂ crystal from a slow acoustic wave, which is characterized by extraordinarily high acoustooptic quality. Modulators of the zeroth diffraction order, modulators of the first Bragg’s order, and a polarization-insensitive deflector are considered. The developed systems ensure the control of the polarization state of optical radiation. These systems are employed in setups and devices based on high-power solid-state and fiber lasers with a wavelength of 1.06 μm.     

Waveguide acoustooptic devices for the real-time spectral analysis of broadband optical signals

Computer simulation and experimental testing of the main characteristics of a waveguide acoustooptic device for the real-time spectral analysis of broadband optical signals are discussed. A mathematical model of such a device is similar to the experimentally tested mathematical model of a waveguide acoustooptic spectral analyzer of radio signals. Two modifications of the spectrum analyzer based on Y-cut lithium niobate are developed and numerically studied. These modifications make it possible to process broadband optical signals in the red and IR ranges. The parameters of the devices are chosen based on real technological and topological requirements for the elements. Comparative analysis shows that the theoretical data on the first modification are in good agreement with the corresponding experimental results.