共查询到19条相似文献,搜索用时 62 毫秒
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主要针对目前SOI(Silicon-on-insulator)纳米光波导结构弯曲损耗严重的问题,系统地进行了理论仿真分析,设计出最佳的纳米波导结构,并采用MEMS工艺对其进行加工制备与优化处理。后利用了SEM(扫描电子显微镜)、AFM(原子力显微镜)、透射谱功率法等研究手段精确测试了在高纯氮退火和BOE腐蚀后处理不变的情况下,不同温度热氧化退火处理下的波导侧壁粗糙度和对应的弯曲损耗,结果表明:波导的侧壁粗糙度随退火温度的变化近似呈二次抛物线变化趋势,在900℃附近达到最低值2.1 nm,对应的半径15μm的环形波导的弯曲损耗为(0.0109±0.001)dB/turn,其损耗值与理论分析结果一致。利用这一结论就可以通过选择不同的优化处理条件来减小环形波导的弯曲损耗,从而实现光能量的高效传输。 相似文献
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光切法在动态表面粗糙度检测中的应用 总被引:1,自引:0,他引:1
应用光切显微镜、CCD摄像机、虚拟仪器和图像处理技术开发了表面粗糙度动态检测系统,利用光切法获得运动表面形貌,再使用图像处理技术提取轮廓特征计算评定参数。通过与触针式仪器进行测量对比实验,论证了检测系统能达到较高的精度。应用检测系统进行了动态检测实验,分析了样本表面的振动和运动速度对检测系统的影响。实验证明,在被测表面的振动幅度小于景深的前提下,该图像检测系统能够应用于动态检测表面粗糙度,适用的速度范围可达到:0 ̄2000rpm(3.14m/s)。 相似文献
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退火质子交换铌酸锂光波导是一类重要的光波导.对采用该技术制备的,具有余弦型弯曲的Y分支光波导,利用宽角有限差分光束传播法,就过渡区长度、波导折射率增量、掩模版开口宽度等对波导弯曲损耗的影响进行了研究,并与余弦型弯曲波导进行了比较.结果表明,Y分支波导和余弦型弯曲波导的弯曲损耗,随波导结构参数的变化基本上是相同的,但二者的表现并不完全一致,因而对Y分支波导结构参数的选择,不能完全依赖于余弦弯曲波导结构的优化.数值结果为相应波导器件的设计和制备提供了一定的参考. 相似文献
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高折射率的LiNbO3光波导,构成四层高折射率波导表面等离子共振传感器.采用传输矩阵方法得基模TM模色散表达式,研究了光波导有效折射与样品折射率之间的关系、光波导传输常数和波长的关系,由表面等离子体波共振耦合条件,得到不同样品折射率的表面等离子共振波长.利用菲涅耳的反射率公式,计算了四层结构波导传感器的透射谱,得到表面... 相似文献
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采用纳米压印微复制技术方法,研制了一种新型的聚合物柔性光栅光波导敏感器件,该器件可用于介入式医用导管的微弯挠曲监测或类似场合的微变形监测.重点阐述了聚合物柔性光栅光波导器件的微复制模具和器件微复制的工艺方法,并对制备工艺技术中的关键技术问题进行了讨论,讨论了测试光纤耦合一体化光栅波导器件的工艺方法.最后利用硅微模具和紫外固化介质材料,成功制备出了截面尺寸为4 μm×20 μm、光栅周期为0.75 μm的聚合物柔性光栅光波导器件. 相似文献
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光波导器件计算机辅助分析系统 总被引:2,自引:0,他引:2
介绍了一个光波导器件计算机辅助分析系统,该系统集成了3个实用工具:光波导有效折射率计算工具,光波导模式求解工具和三维复折射率全矢量有限差分束传播法模拟工具,本系统用于线性波导器件,模拟光在波导中的传播过程,从而可以优化设计波导器件,探索新结构器件。 相似文献
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Low loss and broadband transition between substrate integrated waveguide and rectangular waveguide 下载免费PDF全文
In this article, a novel transition between substrate integrated waveguide (SIW) and rectangular waveguide is proposed. A pair of antipodal tapered probes is developed to convert the E‐field of SIW to that of waveguide, acting as an antipodal dipole antenna to improve the performance of the SIW‐to‐waveguide transition. A back‐to‐back prototype of the proposed transition is fabricated and measured, the results show that the transition achieve a bandwidth of 51.1% from 23.7 to 40 GHz, and a size reduction of 75.3% compared to the SIW‐to‐waveguide transition using antipodal fin‐line. A tolerance analysis is performed via the simulation to verify the reliability of this transition design. For further validation, the antipodal tapered probes are employed for the design of partially filled SIW‐to‐waveguide transition. From its experimental results, it demonstrates that the loss of a single SIW‐to‐waveguide is less than 0.26 dB over the frequency range of 24.9–40 GHz. In addition, such proposed SIW‐to‐waveguide transition is suitable for hermetic packaging due to the inherent property in transition structure. These results show that the proposed transition can offer the advantages of broad bandwidth, low loss, compact size, and stable performance at millimeter‐wave frequencies. © 2015 Wiley Periodicals, Inc. Int J RF and Microwave CAE 26:54–61, 2016. 相似文献
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一体化粗糙度测量传感器的设计 总被引:1,自引:0,他引:1
以表面粗糙度测量仪为例,结合传感器的发展趋势,研究了粗糙度测量传感器的模数一体化实现方法.该传感器将电荷放大、电压幅值放大、A/D转换、数字滤波、数据通信集中在一起,通过DSP实现粗糙度测量过程中数字滤波.结果表明,一体化粗糙度测量传感器集成度高、功能全,提高了数据处理效率,减轻了后续处理电路的计算量. 相似文献
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Analysis and optimization of surface roughness in the ball burnishing process using response surface methodology and desirabilty function 总被引:1,自引:0,他引:1
Aysun Sagbas 《Advances in Engineering Software》2011,42(11):992-998
In the present study, an optimization strategy based on desirability function approach (DFA) together with response surface methodology (RSM) has been used to optimize ball burnishing process of 7178 aluminium alloy. A quadratic regression model was developed to predict surface roughness using RSM with rotatable central composite design (CCD). In the development of predictive models, burnishing force, number of passes, feed rate and burnishing speed were considered as model variables. The results indicated that burnishing force and number of passes were the significant factors on the surface roughness. The predicted surface roughness values and the subsequent verification experiments under the optimal conditions were confirmed the validity of the predicted model. The absolute average error between the experimental and predicted values at the optimal combination of parameter settings for surface roughness was calculated as 2.82%. 相似文献
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