集成光学 集成光学、波导理论

TN252 2005053598 两种不同Y分支光波导的弯曲损耗研究=Bending loss of two kinds of Y-branch optical waveguides[刊,中]／郑宏林 (电子科技大学宽带光纤传输与通信网技术教育部重点实 验室.四川,成都(610054)),陈福深∥半导体光电．- 2005,26(1)．-30-33 针对低损耗S型弯曲Y分支的分析与设计,分别用弯 曲损耗理论和有限差分光束传输法分析了两种不同的S 型弯曲Y分支的损耗特性,比较了不同的波导宽度、分支 间距和分支张角对波导输出损耗特性的影响,得出了一组 最优化的Y分支波导设计参数。图5参5(严寒)     

4通道交叉型二氧化硅光波导延迟线阵列的设计与制备

设计并制备了一种高集成度、低成本、低损耗4通道交叉型二氧化硅光波导延迟线阵列。利用BPM软件对交叉结构光波导延迟线的Y分支的损耗、弯曲损耗进行数值模拟。综合考虑器件尺寸和损耗参数,设计交叉型延迟线结构的弯曲半径最小为1 500 μm,引入优化的锥口Y分支结构和垂直相交波导结构。采用标准半导体制作工艺制备器件,测试得到了器件的红外输出光斑,延迟线延迟时间分别为0、113、226和339 ps。4通道二氧化硅延迟线阵列能实现相邻通道相等的延迟时间间隔,且可通过集成实现延迟时间的增加,同时输出端可以与光纤阵列集成。     

小型铌酸锂多功能集成光学器件

为满足小型光纤陀螺对光学器件小体积的要求,对铌酸锂多功能集成光学小型化器件的结构做了分析和优化设计。采用BPM软件分析了Y形分支波导的S形波导损耗与弯曲长度及折射率差的关系。通过调整退火质子交换的工艺参数,增加了波导对光的束缚能力;降低了小型化芯片上S形波导的弯曲损耗;去掉了原有Y形波导的输出端直波导,直接由S形弯曲波导引至输出端,在更短的芯片上得到了更长的弯曲过渡区。设计制作的芯片长度由常规的20 mm减至12.5 mm,封装后的器件长度减小到20 mm,为目前同类常规器件尺寸的2/3。设计制作的器件插入损耗典型值小于2.5 dB,全温损耗变化量小于0.2 dB。     

弯曲波导研究进展及其应用

本文主要分析了弯曲波导损耗机理,包括传输损耗、辐射损耗、模式转换损耗。重点综述了设计低损耗弯曲波导的方法,包括波导材料、弯曲波导的曲线形状、波导种类、脊型波导的宽度、脊高、弯曲半径、模场分布、弯曲波导曲线形状和其他新型波导结构等。简要概括了近年来设计和制备低损耗弯曲波导的代表性工作。介绍了弯曲波导在集成光学中的应用。通过对弯曲波导的损耗及耦合机制理论的不断完善,实现光在较小弯曲半径的低损耗传输,从而提高集成光学的集成度是弯曲波导今后的发展趋势。     

新型低损耗氧化硅Y分支光波导

提出了一种新型的Y分支光波导结构。该Y分支波导由一个人射波导,一个过渡波导和一对出射波导组成。过渡波导用于改善放射基模与出射偶对称模之间的场分布匹配,有效地提高了功率耦合效率,降低了分支耦合损耗,波束传播法（BPM）数字模拟计算表明,该结构在1．31μm和1．55μm波长下可分别达到0．041dB和0．052dB分支耦合损耗。实验中用等离子化学汽相沉积（CVD）技术制备了SiO2分支波导样品,在上述两波长下分别测得分支耦合损耗为0．08dB和0．09dB,基本达到了设计指标。     

带有矩形过渡区的非对称Y分支光波导

提出了带有矩形过渡区的非对称Y分支光波导的两种设计方案。分别通过设置两分支波导不同的宽度和改变分支波导与矩形中心的轴偏移量,去获得非对称分支比。采用有限差分光束传播法（FD-BPM）对两种结构进行模拟,得出它们的分支比和损耗。分支比分别最高可达809／6和72．9％,其相对应的损耗分别低于0．12dB和0．23dB,充分证明了方案的可行性,为以后非对称Y分支光波导的制作提供了实验基础。     

新型非对称Y分支波导设计与分析

非对称型Y分支波导是用于实现分支波导光功率非均分输出的重要单元器件,在集成光子器件中有广泛应用.基于全内反射原理,提出了一种新型非对称Y分支波导,通过将左右分支波导相对于输入波导在横向方向上进行偏移以实现特定分束比光输出,并对其光学特性进行模拟分析.结果表明,该波导结构不仅能实现任意特定分束比光输出,在分支角达到14°条件下其输出损耗仅为0.417 dB,而且偏振依赖性低、工艺制作难度小,这种新型非对称Y分支波导在集成光子器件中具有重要应用意义.     

基于MIM型表面等离子体光波导的Y形分束器的传输特性研究

采用二维时域有限差分(FDTD)法,分析并对比了弯曲分叉部分的形状分别为正弦形和圆弧形的基于金属-绝缘体-金属(MIM)型表面等离子体光波导的Y形分束器的反射率、传输率以及能量分束比随几何结构参数的变化关系。数值计算表明,波导宽度对这两种Y形分束器传输特性的影响较为明显,两个输出分支的偏移量和弯曲分叉部分的长度对这两种Y形分束器传输特性的影响比较微弱。在600～1500nm波长范围内,弯曲分叉部分为圆弧形的Y形分束器的传输特性比弯曲分叉部分为正弦形的好。对于非对称型Y形分束器,当弯曲分叉部分为正弦形时,偏移量对反射率、传输率和能量分束比的调节作用较为明显,能量分束比最大可达到2∶1。当弯曲分叉部分为圆弧形时,偏移量对反射率、传输率和能量分束比的调节作用较为微弱。     

基于光纤反射腔的高灵敏电流传感器方案

提出了一种基于平面Y分支波导与法拉第旋镜的高灵敏度光纤电流传感器结构方案。利用两个法拉第旋镜与平面Y分支波导构成一个光纤反射腔,通过光在腔中的多次反射来增加待测电流导致的传感光纤中的法拉第相移,从而实现对微弱电流的测量。该结构方案中首次采用了平面Y分支光波导,从而可降低光路系统损耗,增加灵敏度,为微弱电流测量的工程化提供了一种可行的方法。     

基于光纤反射腔的高灵敏电流传感器方案

提出了一种基于平面Y分支波导与法拉第旋镜的高灵敏度光纤电流传感器结构方案。利用两个法拉第旋镜与平面Y分支波导构成一个光纤反射腔,通过光在腔中的多次反射来增加待测电流导致的传感光纤中的法拉第相移,从而实现对微弱电流的测量。该结构方案中首次采用了平面Y分支光波导,从而可降低光路系统损耗,增加灵敏度,为微弱电流测量的工程化提供了一种可行的方法。     

BPM Simulation and Comparison of 1 × 2 Directional Waveguide Coupling and Y-Junction Coupling Silicon-on-Insulator Optical Couplers

For developing large area opto-electronic silicon-on-insulator (SOI) devices, the optical coupler is a basic key device. In this article, the authors design and simulate 1 2 2 directional waveguide coupling and Y-branch coupling optical couplers based on Unibond SOI rib waveguides. The beam propagation method (BPM) is used for light propagation analysis. The simulation results and comparisons of the two kinds of optical couplers are reported. The S-bend waveguide for attaching to the two kinds of SOI optical coupler is also analyzed by BPM. We find that the directional coupler has lower power loss, but the Y-junction coupler is more wavelength insensitive with the same device size and splitting angle. The fabrication tolerance analysis shows Y-junction coupler has better fabrication characteristics.     

数值模拟二维间隙表面等离子波导传输特性

利用表面等离子激元的新颖特性,设计了二维间隙表面等离子波导.以这种结构为基础通过变形和组合形成90°直角弯曲波导、T型光功率分配器和光开光,采用时域有限差分法研究了它们的传输特性.结果表明:不同于介质光波导的弯曲损耗来自于辐射泄漏,90°直角弯曲间隙表面等离子波导的能量损耗主要来自于金属中的欧姆热损耗.在间隙达到40 nm以上后,当直行段的长度适当时,弯曲段的透射率较相同长度的直波导的透射率要大.T型光功率分配器在两输出波导的间隙宽度比达到0.6及以上时,不同于传统介质波导的分光原则,能量主要沿等效折射率较小的输出臂流出.当两输入光的相位反相时,T型光开关处于输出截止的状态,当两输入光的相位同相时,T型光开关处于输出导通的状态.所有波导间隙均小于衍射极限,实现了超衍射极限传播,可用于未来了超大规模集成光路中.     

Fabrication of 1×2 asymmetric plastic optical fiber coupler for portable optical access-card system

We proposed a simple low-cost acrylic and metal-based Y-branch plastic optical fiber (POF) splitter which utilizes a low cost optical polymer glue NOA63 as the main waveguiding medium at the waveguide taper region. The device is composed of three sections: an input POF waveguide, a middle waveguide taper region and output POF waveguides. A desktop high speed CNC engraver is utilized to produce the mold inserts used for the optical devices. Short POF fibers are inserted into the engraved slots at the input and output ports. UV curable optical polymer glue NOA63 is injected into the waveguide taper region and cured. The assembling is completed when the top plate is positioned to enclose the device structure and connecting screws are secured. Both POF splitters have an average insertion loss of 7.8 dB, coupling ratio of 55: 45 and 57: 43 for the acrylic and metal-based splitters respectively. The devices have excess loss of 4.82 and 4.73 dB for the acrylic and metal-based splitters respectively.     

Acrylic and metal based Y-branch plastic optical fiber splitter with optical NOA63 polymer waveguide taper region

We proposed a simple low-cost acrylic and metal-based Y-branch plastic optical fiber (POF) splitter which utilizes a low cost optical polymer glue NOA63 as the main waveguiding medium at the waveguide taper region. The device is composed of three sections: an input POF waveguide, a middle waveguide taper region and output POF waveguides. A desktop high speed CNC engraver is utilized to produce the mold inserts used for the optical devices. Short POF fibers are inserted into the engraved slots at the input and output ports. UV curable optical polymer glue NOA63 is injected into the waveguide taper region and cured. The assembling is completed when the top plate is positioned to enclose the device structure and connecting screws are secured. Both POF splitters have an average insertion loss of 7.8 dB, coupling ratio of 55: 45 and 57: 43 for the acrylic and metal-based splitters respectively. The devices have excess loss of 4.82 and 4.73 dB for the acrylic and metal-based splitters respectively.     

基于表面等等离波子的新型Y分支波导

新型高效的纳米光波导器件的研制纳米集成光学的核心技术之一。Y分支波导作为最基本的分光和光路连接元件是纳米光学器件设计与制备的基础。运用时域有限差分(FDTD)法,模拟计算了基于表面等等离波子(SPP)的纳米Y分支波导的传输特性。结果表明,该新型Y分支波导在光通信波段可以实现大角度的分光功能,且在180°分支情况下,传输效率仍高达92.8%以上。另外,该波导还具有导波性能良好、对分叉处间隙缺陷大小不敏感及制作容差较大和器件尺寸在纳米量级等特点。对该新型光波导器件的研究为未来纳米集成光学器件的研制和应用有一定的指导意义。     

Analysis of electrooptically induced waveguides in strontium barium niobate and optical modulators

An electrooptically induced optical waveguide can be formed by applying a DC voltage between electrodes fabricated on the surface of a crystal with strong electrooptic coefficients (for example, strontium barium niobate). Calculations of the refractive index profile and the optical mode size for such waveguides are presented. Approximate solutions for the fundamental mode are used to analyse the power coupling between a single-mode step-profile fibre and these waveguides. The power transmission losses in the straight and S-shaped waveguides are estimated by using a finite-difference beam propagation method (FD-BPM). The calculations predict that a new kind of modulator/switch can be realized with the induced waveguides. The important characteristics of these devices are discussed and compared with LiNbO₃ optical waveguide modulators.     

基于非对称脊波导的多种聚合物弯波导性能分析

以缩短马赫-曾德尔(M-Z)电光调制器分支波导为目的,将有机聚合物非对称结构的脊波导应用于S弯波导中。采用半矢量有限差分光束传输分析法,系统地分析了不同参数下采用非对称脊波导的三种常见弯波导,即正弦弯、圆弧弯和余弦弯分支波导的TM00光场传输损耗,并与采用对称脊波导的结构相比较。研究表明,在芯层厚度h=1.5μm、脊高为0.3μm、脊宽w=4μm、分支高度G=11μm的情况下,当脊波导短边芯层平板宽度s≥2μm时,在相同传输损耗条件下,正弦弯、圆弧弯和余弦弯分支波导长度分别可减少40%、30%和25%,该结果对有机聚合物M-Z调制器中分支波导的设计具有一定的参考价值。     

Light-propagation characteristics of Y-branch defect waveguides in AlGaAs-based air-bridge-type two-dimensional photonic crystal slabs

Y-branch defect waveguides (DWGs) in an AlGaAs-based air-bridge-type two-dimensional (2D) photonic crystal (PC) slab were fabricated, and the resulting optical transmission spectra were measured. Optical beam propagation along the waveguide was successfully observed in vidicon IR images. The measured transmission spectra at the two output ports in the Y-branch DWG were remarkably similar in shape and magnitude. From comparison between the measured and calculated transmission spectra, the observed optical beam was identified as the guided mode based on the Y-branch DWG in the 2D PC slab. The results suggest that the Y-branch DWG used in the experiment has the potential to function as an ultrasmall 3-dB beam splitter with good performance.     

Ultralow-bending-loss surface-plasmon-polariton waveguides

We report the transmission, reflection and loss properties of 90-degree and 135-degree bent silicon waveguide and 90-degree and 135-degree bent surface-plasmon polariton (SPP) waveguides composed of metal thin film and silicon. Finite difference time domain simulation analysis shows that the maximum bending transmittances of 90-degree bent and 135-degree bent silicon waveguides are 51% and smaller than 10%, respectively, and the maximum bending transmittances of 90-degree bent and 135-degree bent SPP waveguides are 80% or so, and they are higher 30% and 70% than that of identically-bent silicon waveguides, respectively. Moreover, the SPP waveguide bend with metal thin film as inner layer of the bend and silicon as outer layer of the bend has much higher transmission than ones with silicon as the inner layer and metal thin film as the outer layer. The waveguide bend with metal as the inner layer and dielectric as the outer layer will be potential for integrated photonic devices and subsystem.