共焦波导结构回旋行波管的设计与仿真

针对0.14 THz大气窗口,利用CST微波工作室和3维粒子模拟软件,对共焦波导结构的太赫兹回旋行波管进行了冷腔色散和注波互作用的模拟研究。以TE06模式作为互作用工作模式,在电压为35 kV、电流为2 A、横纵速度比为0.85的电子束参数下,当输入信号为1 W时,得到最高2 kW的微波功率输出,3 dB带宽为3.5 GHz,增益为30 dB。     

Femtosecond laser microstructuring: an enabling tool for optofluidic lab‐on‐chips

This paper provides an overview of the rather new field concerning the applications of femtosecond laser microstructuring of glass to optofluidics. Femtosecond lasers have recently emerged as a powerful microfabrication tool due to their unique characteristics. On the one hand, they enable to induce a permanent refractive index increase, in a micrometer‐sized volume of the material, allowing single‐step, three‐dimensional fabrication of optical waveguides. On the other hand, femtosecond‐laser irradiation of fused silica followed by chemical etching enables the manufacturing of directly buried microfluidic channels. This opens the intriguing possibility of using a single laser system for the fabrication and three‐dimensional integration of optofluidic devices. This paper will review the state of the art of femtosecond laser fabrication of optical waveguides and microfluidic channels, as well as their integration for high sensitivity detection of biomolecules and for cell manipulation.     

叠层荧光集光太阳能光伏器件的性能模拟和优化

荧光集光太阳能光伏器件可以减少太阳能电池的用量,有效降低光伏发电的成本.相对于单层荧光 集光太阳能光伏器件,叠层荧光集光太阳能光伏器件能分波段充分利用太阳光谱,提高荧光集光太阳能光伏 器件的效率,进一步降低光伏发电的成本.但是,叠层荧光集光太阳能光伏器件涉及较多的参量,难以通过实验 优化.本文分析了从单层到叠层荧光集光太阳能光伏器件的全部物理过程,建立了数学模型,并相应编制了 计算机模拟软件.运用上述软件,系统研究了器件尺寸、太阳能电池的带隙对光电转换效率的影响.     

GaP波导型发射器产生频率可调谐太赫兹脉冲

报道了利用脉宽可调的光子晶体光纤飞秒激光放大器抽运矩形波导结构的GaP晶体太赫兹(THz) 发射器产生频率可调谐的超快THz脉冲.非线性晶体中光整流过程产生的THz辐射频率随抽运光脉冲宽度而 变化. GaP波导THz发射器可通过波导的几何尺寸来控制色散,以达到增加有效作用长度和提高输出功率的目的. 不同横截面尺寸的波导型发射器的THz辐射峰值频率随相位匹配条件的改变而改变,加以脉宽调节技术, 可以在大频谱范围获得频谱精细可调的THz脉冲.实验中在1 mm×0.7 mm的波导型THz发射器中获得了 频率可调谐的THz脉冲.提出实现THz辐射频率大范围调谐的GaP波导型阵列发射器的实施方案.     

纳米银线波导中表面等离极化波激发和辐射的偏振特性研究术

在可见光波段（λ=750nm）,实验研究了在端面辅助情况下,细纳米银线波导中表面等离极化波激发和辐射的偏振特性．实验发现在细纳米银线中,不同偏振态的入射光对应的表面等离极化激元的激发和传输效率有明显不同,但对应的出射光始终为方向恒定的线偏振光．对于化学合成的纳米银线,端面的轴对称性普遍比较好,对此类纳米银线进行激发时,如果入射光偏振态与纳米线近似平行,则激发和传输表面等离极化激元的效率最高;如果正交,激发和传输效率则最低．对于某些端面轴对称性较差的纳米银线,如端面为尖端或类斜面,当入射光偏振态与纳米线有一定夹角时,激发和传输表面等离极化激元的效率最高．在入射光偏振改变的过程中出射光的偏振方向始终与纳米银线平行．最后结合有限元差分方法理论解释了纳米银线中这种偏振特性的物理机理．利用纳米银线中表面等离极化激元激发和辐射的偏振特性,可以在亚波长尺寸上实现对光强和偏振态的调控．     

一种基于机器视觉的平面光波导器件封装手动耦合系统

对平面光波导器件封装手动耦合系统进行了改进,增加了3个黑白摄像头,3张AV转USB采集卡,通过采集卡采集对准图像,利用LabVIEW8.2和IMAQ vision软件编程,将图片进行BCG调节、反转、闭合、边缘提取、手动阈值、形态学变化、直线拟合等一系列处理和识别后,实现了对光波导分路器与输入、输出光纤阵列的平行度和像素距离的检测,以一个熟练工封装132路平面光波导来说平均节省了对接封装时间10 min,减少了操作者的劳动量,减小了对准损耗,减小了人为误差。     

折叠半模基片集成波导在滤波器和均衡器中的应用

提出了一种数学建模方法用来分析折叠半模基片集成波导(FHMSIW)结构的场分布。基于多线理论首次计算了FHMSIW结构的衰减常数和相位常数,验证其与传统波导和基片集成波导的等效性。提出了FHMSIW结构具有高通特性和带阻特性,同时该结构的上下层具有近似奇对称的性质。通过在FHMSIW结构的中间金属层蚀刻缝隙或者添加金属过孔,就可以实现器件由带通到带阻的性能转换,给出了FHMSIW结构带阻、带通特性的产生和变换机理。利用其独特的性质,分别设计了等效HMSIW四分之一谐振枝节加载的FHMSIW均衡器和FHMSIW带通滤波器,设计的FHMSIW均衡器无需附加额外的馈电机制。测量结果显示出器件具有良好的性能,与仿真结果具有很好的一致性。相比于其他的平面电路,该设计的结构具有小型化、低损耗以及高Q值等优势。     

半波长超导共面波导谐振腔传输及温度特性研究

超导共面波导谐振腔主要包括四分之一波长型和半波长型.本文对半波长超导共面波导谐振腔使用并联RLC电路进行等效分析,使用sonnet软件进行仿真其传输特性,通过电子束蒸发和激光直写等工艺制备出样品,在低温超导状态下使用矢量网络分析仪对其传输特性进行测量,以及通过持续降温方式研究其传输特性受温度的影响.实验表明:测得的谐振频率和外部品质因数与设计值吻合;谐振频率受动态电感的影响随温度降低而升高;外部品质因数随温度降低而保持基本不变;内部品质因先受导体损耗的影响随温度降低而急剧升高,当温度降低至一定温度后内部品质因数受介电损耗的影响随温度降低而保持基本不变;总品质因数在温度较高时主要来自于导体损耗,在温度较低时主要来自于介电损耗和外部品质因数,随温度的变化趋势和内部品质因数一致.     

Nanoscale C‐Rich SixC1−x Bus/Ring Waveguide Based Cross‐Wavelength Data Converter

The carbon‐rich silicon carbide (C‐rich Si_xC_1?x) micro‐ring channel waveguide with asymmetric core aspect is demonstrated for all‐optical cross‐wavelength pulsed return‐to‐zero on‐off keying (PRZ‐OOK) data conversion. Enhanced nonlinear optical Kerr switching enables 12‐Gbit per second data processing with optimized modulation depth. The inverse tapered waveguide at end‐face further enlarges the edge‐coupling efficiency, and the asymmetric channel waveguide distinguishes the polarization modes. To prevent data shape distortion, the bus/ring gap spacing is adjusted to control the quality factor (Q‐factor) of the micro‐ring. Designing the waveguide cross section at 500 × 350 nm² provides the C‐rich Si_xC_1?x channel waveguide to induce strong transverse electric mode (TE‐mode) confinement with a large Kerr nonlinearity of 2.44 × 10^?12 cm² W^?1. Owing to the trade‐off between the Q‐factor and the on/off extinction ratio, the optimized bus/ring gap spacing of 1400 nm is selected to provide a coupling ratio at 5–6% for compromising the modulation depth and the switching throughput. Such a C‐rich Si_xC_1?x micro‐ring with asymmetric channel waveguide greatly enhances the cross‐wavelength data conversion efficiency to favor its on‐chip all‐optical data processing applications for future optoelectronic interconnect circuits.     

The Scattering Problem in PT‐Symmetric Periodic Structures of 1D Two‐Material Waveguide Networks

A PT‐symmetric periodic structure with two‐material waveguide networks is constructed. In this study, how changing the number of cells affects the transmission properties is investigated. The results show that the PT‐unbroken (broken) region of the system is only determined by the cell structure, regardless of the number of unit cells. This means that any system has the same exceptional points (EPs), regardless of the number of cells and as long as the cell structure is consistent. In addition, it is confirmed that the coherent perfect absorbers and lasers (CPA lasers) occur in our model. The transfer matrix method is used to derive a sufficient condition for achieving the CPA laser point. A simple, effective formula for predicting the CPA laser state in an N unit cell system is derived.