包含左手材料的四层平板波导中的光导模

研究一个芯子层是左手材料,其他三层由传统材料构成的四层平板光波导系统,利用图解法对各种TE偏振的导波模式的解进行详细分析.研究表明,四层左手材料光波导既能支持振荡导模,也能支持表面导模,与三层左手材料光波导相比较,此四层波导的导波模式呈现一些新的特性.对于中间传统材料层存在振荡场的情形:芯子层支持振荡导模的光波导中存在基模,并且高阶振荡导模出现模式缺失的性质;芯子层支持表面导模的光波导可以支持基模和多个高阶模式,并且存在模式兼并的性质.对于中间传统材料层存在衰减场的情形,此四层波导结构可等效为三层左手材料光波导.这些新的光波导传输性质对各种光波导器件的制作有潜在的应用价值.     

含单负材料的不对称平板波导的传导模

利用图解法系统地研究了由不同类型的单负材料作为包层的三层平板波导的模式特征.研究表明单负介质波导具有一系列奇异的特性,与传统介质波导或左手介质波导相比,此波导的芯区横向振荡导模的模折射率范围较大.除0阶导模外,其它TE,TM导模均为芯区横向振荡模,且同阶的TE、TM模的色散曲线几乎重合,只有0阶的TE,TM模才可以支持表面波的传播.单负介质的结构参数对0阶导模的影响较大.一定条件下,波导中可以出现0阶导模的完伞缺失或仅支持表面波的传输,还会出现超慢波现象,甚至可以共生都是后向波的0阶双模.     

电压调控多种金属膜波导特性研究

采用自由空间耦合的方法,激发双面金属包覆波导中的超高阶导模,通过在双面金属包覆介质波导的两个金属膜上加不同的电压,改变导波层铌酸锂的厚度和折射率,得到不同参数下的衰减全反射谱,从而验证超高阶导模的偏振不灵敏性及对导波层厚度和折射率十分灵敏的特殊性质,实验结果与理论相吻合。比较相同条件下反射率的变化,得到铝包覆波导的灵敏度要高于金包覆波导。所得结果对集成光电子器件的研制有一定的参考价值。     

基于古斯-汉欣位移效应的波长传感研究

利用双面金属包覆波导在导模共振激发时对古斯-汉欣位移具有极大的增强效应来实现激光波长微小变化的监测.双面金属包覆波导由上层金膜、导波层和下层金膜组成.当导波层厚度为亚毫米尺度时,应用自由空间耦合技术使入射的激光以小角度入射,在满足相位匹配的条件下激发超高阶导模.理论研究表明,当波导的辐射损耗等于本征损耗时,反射光的侧向位移可达到数百微米,并且此时激发的超高阶导模对波长具有极强的色散能力.通过测量反射光的侧向位移可实现对激光波长变化的实时探测,且具有很高的灵敏度.同时,实验中探测信号只与光束位置相关,可有效避免因光源输出光强的波动带来的干扰.实验测量结果表明对激光波长在859nm附近的分辨率可达到0.2 pm.     

基于古斯-汉欣位移效应的波长传感研究

利用双面金属包覆波导在导模共振激发时对古斯-汉欣位移具有极大的增强效应来实现激光波长微小变化的监测.双面金属包覆波导由上层金膜、导波层和下层金膜组成.当导波层厚度为亚毫米尺度时,应用自由空间耦合技术使入射的激光以小角度入射,在满足相位匹配的条件下激发超高阶导模.理论研究表明,当波导的辐射损耗等于本征损耗时,反射光的侧向...     

平面光波导用于实时测试生化反应新方法的研究

在分析经典消逝波光波导生化传感器的基础上,为寻找性能更佳的传感器,探讨用更为直观的截止特性来进行生化传感。分别对三层及四层平板波导进行了研究,指出了作为基于截止特性的生化传感器三层波导结构存在的局限性。在理论上研究了可以在四层波导中使用变折射率材料来进行基于截止特性的生化传感,并给出了由空气隙、极化聚合物、高折射率薄膜、待测物组成的传感器结构示意图。用数值分析的方法绘出了此装置的灵敏度与高折射率薄膜厚度的关系曲线,并将它同经典消逝波光波导生化传感器灵敏度与薄膜厚度关系图进行了比较。结果表明,这种新型传感器理论上可以在较厚的薄膜结构中达到很高的灵敏度。     

光波导氨敏传感器的研究

提出了一种新型的光波导氨敏传感器,将光波导中消逝波理论与纳米多孔薄膜技术相结合,在玻璃薄膜光波导上制备一层纳米TiO2多孔薄膜,并将氨敏试剂（BTB）固定在纳米TiO2多孔薄膜中,利用导波光的消逝场实时地探测敏感薄膜对导波光的吸收,实现了对氨气的探测,检测下限达到1ppm。同时对比了致密敏感薄膜和多孔敏感薄膜对氨气的响...     

小球藻溶液浓度与吸收系数的同时测量

为得到高准确度的小球藻浓度,利用空芯金属包覆波导作为测量腔对小球藻进行测量.利用自由空间耦合技术激发含有小球藻溶液的空芯金属包覆波导中超高阶导模,通过检测超高阶导模的衰减全反射吸收峰位置和反射极小值Rmin的变化,实现了小球藻溶液浓度和吸收系数的同时测量.该方法不仅可检测10-9 mol量级的小球藻浓度,而且具有测量成本低、操作方便等优点.     

集成光学 集成光学、波导理论

TN252 2006043277亚毫米尺度双面金属波导的超高阶模及其滤波特性研究=Research of ultrahigh-order modes in double metal-clad-ding optical waveguide with submilli meter scale[刊,中]/曹庄琪(上海交通大学物理系,导波光电子器件实验室.上海(200240)) ,陆海峰…∥光学学报.—2006 ,26(4) .—497-500利用真空溅射法在一片亚毫米尺度的光学玻璃平板两面分别镀上不同厚度的金属薄膜,构成一种超厚的双面金属包覆波导,采用自由空间耦合技术实现了这种波导中超高阶导模的激发。由于超高阶导模具有对波长特别灵敏而对偏振不灵敏的特殊性质,…     

波导型钯(Pd)膜氢传感器数值模拟及优化

基于离子交换波导的集成型器件是氢敏传感器中很有发展潜力的一种. 传感区域由离子交换波导及其表面的金属钯膜组成, 通过有限差分法（FDM）计算了这种波导结构中的导模及表面等离子模的模场分布, 分析了其传播特性与钯膜光学常数的关系, 并结合束传播方法（BPM）对钯膜的厚度进行了优化, 使其具有最高的灵敏度.     

Slab waveguide with air core layer and anisotropic left-handed material claddings as a sensor

A three-layer slab waveguide with air core layer and anisotropic left-handed material claddings is investigated for sensing applications. Different from the waveguide mode sensors and surface plasmon resonance sensors in which the analyte is placed in the evanescent field region, the proposed sensor contains the sample in the core region that supports the oscillating field. Due to the strong concentration of the electromagnetic field in the analyte medium, the proposed device exhibits unusual sensitivity enhancement. The simulations revealed that the sensitivity improvement of TE₃ mode compared to conventional evanescent wave sensor is approximately a factor of 20.     

一种新型的振荡场光化学传感器

利用法布里珀罗振荡模构造了一种新型的光化学传感器。与传统的以表面等离子模和光导模为探针的迅衰场传感器不同 ,这种新型结构中被传感介质处于法布里珀罗腔的振荡场中 ,其能量在全部入射光能中的比重占得很大 ,使得这种传感器具有很高的灵敏度。实验证实这类传感器对葡萄糖溶液浓度和折射率的测量精度皆可达 10 - 5数量级以上     

Optical sensors based on Fabry–Perot resonator and fringes of equal thickness structure

We propose theoretically two optical sensor structures based on Fabry–Perot resonator and fringes of equal thickness structure. Different from the conventional slab waveguide sensors in which the sample interacts with the evanescent field in the cladding layer, the proposed sensors contain the sample in the core layer. The first proposed sensor comprises a piezoelectric material as a substrate with the driving potential difference as the sensing probe for refractive index changes of the sample. The second sensor comprises fringes of equal thickness structure with the number of fringes per unit length is the probe for changes in the index of the sample. The calculations reveal that the proposed sensors have high sensitivity to changes in the refractive index of the sample.     

Bimetallic Silver-Gold Film Waveguide Surface Plasmon Resonance Sensor

It is desirable that a surface plasmon resonance (SPR) sensor is highly sensitive to binding interactions within the sensing region, generate evanescent fields with long penetration depths, and utilize a metal film that is very stable even in extreme environmental conditions. In this study, we present the first example of a wavelength-modulated waveguide SPR sensor with a bimetallic silver-gold film for surface plasmon excitation. The underlying silver yields better evanescent field enhancement of the sensing surface, while the overlying gold ensures that the stability of the metallic film is not compromised. It is shown experimentally that in terms of dλ/dn, the bimetallic film waveguide SPR configuration has a sensitivity of 1232 nm/RIU, greater than two times improvement from the 594 nm/RIU achievable with single gold film waveguide SPR sensor. The higher sensitivity, compact nature, and better evanescent field enhancement of this configuration provides the potential to biosensing applications.     

Bimetallic Silver–Gold Film Waveguide Surface Plasmon Resonance Sensor

Abstract

It is desirable that a surface plasmon resonance (SPR) sensor is highly sensitive to binding interactions within the sensing region, generate evanescent fields with long penetration depths, and utilize a metal film that is very stable even in extreme environmental conditions. In this study, we present the first example of a wavelength-modulated waveguide SPR sensor with a bimetallic silver–gold film for surface plasmon excitation. The underlying silver yields better evanescent field enhancement of the sensing surface, while the overlying gold ensures that the stability of the metallic film is not compromised. It is shown experimentally that in terms of dλ/dn, the bimetallic film waveguide SPR configuration has a sensitivity of 1232 nm/RIU, greater than two times improvement from the 594 nm/RIU achievable with single gold film waveguide SPR sensor. The higher sensitivity, compact nature, and better evanescent field enhancement of this configuration provides the potential to biosensing applications.     

Thin Film Waveguide Sensor for Measurement of the Absorption Coefficient of Hemoglobin Derivatives

A simple method for determining the absorption coefficient of oxyhemoglobin and deoxyhemoglobin in human blood is proposed. The method is based on a variation of the complex propagation constant of guided wave in a thin-film optical waveguide. On the waveguide layer, a serial multi-channel sample chamber is constructed to vary the interaction length between the evanescent field and the sample, and the dependence of the sensor response on the interaction length is investigated for various concentrations of two hemoglobins. The response of this sensor is linearly proportional to the interaction length and the concentration of the two hemoglobins. The attenuation constant due to the evanescent field absorption between the channels is experimentally obtained with the designed sensor, and the absorption coefficient is determined by the proposed method. The determined absorption coefficients coincided with those obtained by conventional transmission measurement.     

Spiral-path high-sensitivity silicon photonic wire molecular sensor with temperature-independent response

We demonstrate a new silicon photonic wire waveguide evanescent field (PWEF) sensor that exploits the strong evanescent field of the transverse magnetic mode of this high-index-contrast, submicrometer-dimension waveguide. High sensitivity is achieved by using a 2 mm long double-spiral waveguide structure that fits within a compact circular area of 150 microm diameter, facilitating compatibility with commercial spotting apparatus and the fabrication of densely spaced sensor arrays. By incorporating the PWEF sensor element into a balanced waveguide Mach-Zehnder interferometer circuit, a minimum detectable mass of approximately 10 fg of streptavidin protein is demonstrated with near temperature-independent response.     

Modelling of rib waveguide bends for sensor applications

Wave propagation through curved bends in integrated optical waveguides is governed by the evanescent field and the radiation loss of the eigenmodes. Since these parameters are influenced by the refractive index of the surrounding medium, circular bends in rib waveguides have been successfully employed as chemical sensors for liquids and gases. In this paper the electromagnetic field, the refractive index and the radiation loss of the eigenmodes are precisely determined by a fully vectorial approach based on the method of lines. An axial discretization and Bessel functions of complex order are employed for the rigorous computation of the evanescent field. The intensity distributions of the first modes in a rib waveguide are presented. The influence of the rib height on the sensitivity of the modal index to the refractive index of the surrounding medium is investigated. The results are useful for the optimization of the sensor design.     

Fabrication and study of a metal-clad planar waveguide based biosensor

A metal-clad planar optical waveguide biosensor having five layer structure has been fabricated to study the detection of Pseudomonas and Pseudomonas-like bacteria. This waveguide is designed to increase the overlap of the evanescent field extension from the sensor face with the micro-scale biological objects in the bulk solution, to place most of the entire volume of the bacteria within the evanescent field. The results presented here leads to a significant optimization of the important design parameters to sense micro-scale biological objects. We have compared our computed results with the results obtained by similar non-metallic clad biosensor. The effect of affinity-layer refractive index on the sensitivity of these planar waveguides is also studied. We have shown this for some special cases by obtaining reflection dips at the particular angle of incidence. Our observations show that the metal-clad planar optical waveguide biosensor having higher affinity refractive index will give better sensitivity than other similar non-metallic clad biosensor. The validation of metal-clad planar optical waveguide sensor for the detection of Pseudomonas aeruginosa bacterium is also made.