利用场分布计算单腔微波参量

介绍了利用加速管的场分布计算单腔微波参量的一种方法. 在已知耦合腔链各本征模式的谐振频率和电场分布的条件下，可以通过回路方程组求出耦合腔链的单腔频率和腔间耦合系数. 这种方法给加速管设计和调谐带来了很大帮助，在加速腔数目较多或者结构非均匀的条件下尤为有效.     

不插入探针检测耦合腔链各单腔频率的方法

介绍一种不需插入活塞探针进入耦合谐振腔链, 而由计算机通过微波网络分析仪, 从腔链的输入波导获取通带特性数据, 配以专门的软件, 便可分析求解各单腔频率的方法.     

开放式法布里-珀罗光学微腔中光与单量子系统的相互作用

光与物质相互作用的过程具有丰富的物理内涵,不仅有助于理解光的本质,更可以提供一种有效操控物质的手段.开放式光学微腔具有光场强局域性、频率域和空间域的可调谐性以及光纤可集成性等特点,为研究微腔内的光与物质相互作用提供了一个理想平台.本文首先介绍基于开放式法布里-珀罗微腔的腔量子电动力学系统的基本特性,然后介绍开放式法布里-珀罗微腔结构的制备方法,进而从弱耦合、强耦合和差发射体三方面着重介绍近年来开放式微腔与固态单量子系统相互作用的研究工作,最后进行了总结与展望.     

Ka波段耦合腔行波管放大器设计

由于Ka波段耦合腔行波管放大器设计技术取得了较大的发展,已经可以满足军用雷达的严格要求,这种设计技术也受到更多的关注.这里简要介绍Ka波段耦合腔行波管放大器的设计技术.通过介绍Ka波段耦合腔行波管放大器的基本组成、工作原理及设计中仿真工具的运用来说明这种设计技术.用这种设计技术成功设计出了多种耦合腔行波管放大器,在功率和体积方面突破了原有的Ka波段固态和螺旋线行波管放大器的局限,取得了明显的进步.Ka波段耦合腔行波管放大器的设计技术经过实践验证,在输出功率、带宽及重量方面已经取得了重大突破,满足了现代军用雷达的需求.     

0.3 THz TM10, 1, 0模同轴耦合腔链

通过本征方程研究了工作在太赫兹(THz)频段的高次模同轴谐振腔,讨论了TM_{m, 1, 0}模,TM_{m, 2.0}模与TM_{m, 1, 1}模的谐振频率与腔体的几何参数之间的关系,并给出了工作模式的选择依据。在此基础上,提出了一种新型的0.3 THz TM_{10, 1, 0}模同轴耦合腔链,使用等效电路模型和CST-MWS软件对耦合腔链的色散特性、特征阻抗和电场分布等冷腔特性进行了分析和仿真,并着重分析和总结了耦合腔链的几何参数对色散特性和特征阻抗的影响。研究结果表明:对于工作在THz频段的高次模同轴耦合腔链,采用TM_{10, 1, 0}模为工作模式是合理的选择; 工作于2π腔模的0.3 THz TM_{10, 1, 0}模同轴耦合腔链具有较大的特征阻抗,但模式间隔较小,因此可将其应用于窄带太赫兹扩展互作用器件; 增大高次模耦合腔链的耦合槽张角是增大模式间隔的最佳途径。     

SSC边耦合加速腔的调谐

为缩短边耦合加速腔腔片制造周期，需用部分腔片确定Ｔａｕｋ的π／２模式频率，采用整腔结尾，调节端腔频率使相邻耦合腔输出最小的方法，得到比较准确的结果。焊后调谐，耦合腔频率用近似方法调节，加速腔则用相对精确的方法调谐。用桥耦合器连接Ｔａｎｋ后，腔数增加引起π／２模式频率下降，桥耦合器的频率要调高于设计值。     

基于环形微腔的多频段三角晶格光子晶体耦合腔波导光学传输特性

本文理论研究了近红外波段硅基三角晶格光子晶体环形微腔的光场局域特性,通过将微腔在空间周期性排列组成耦合腔光波导,研究了多个导带区域内光束传输时的群速度,最大和最小值分别为0.0028c和0.00028c.将环形微腔在垂直于光传输方向上进行交错排列,通过改变相邻微腔之间的耦合区域,可以大幅降低多频段范围内光束在耦合腔波导中传输时群速度之间的差异,并提高部分频段的透过率数值.在不改变介质柱半径条件下,通过去掉三角晶格光子晶体中距中心介质柱距离分别为2a和√3a的六个介质柱构成了两种微腔,研究了两种微腔所支持的谐振波长之间的差异,在此基础上构造了两种耦合腔波导,进而将这两种耦合腔光波导与W1型输入/输出波导相连,最终实现了在多个不同频率范围内降低群速度的同时实现频段选择和频段分束功能,其导模群速度可降低到0.00047c.     

双腔光力学系统中输出光场纠缠特性的研究

腔光力学系统中的光辐射压力可以使系统中的各个子系统之间产生量子纠缠,最近在腔光力学系统中的量子纠缠引起了人们广泛的关注.本文研究了双腔光力系统中关于输出光场之间纠缠的性质,发现:此系统中力学振子的弛豫速率和滤波器带宽以及非相等耦合对输出光场之间纠缠的大小有着非常显著的影响,特别是在相等耦合条件下,输出光场中心频率与光腔本征频率近共振时,滤波器带宽对输出光场纠缠有着显著的抑制作用;但是如果采用非相等耦合,则可以有效抵制滤波器带宽对纠缠的抑制作用,使输出光场纠缠得到大幅提高.研究结果可应用在光力耦合系统中实现量子态转换、量子隐形传态等量子信息处理过程.     

非均匀加速结构腔间耦合系数模拟计算

电子直线加速器的聚束段对于会聚入射电子相位,提高电子直线加速器出射束流性能起着至为关键的作用. 而准确计算聚束段腔间耦合系数又是设计聚束段耦合孔几何结构的关键. 本文利用电磁场计算软件MAFIA的特征值计算模块E模块, 分别计算出单腔频率, 双腔腔链的两个本征频率,从而得到聚束段腔间耦合系数. 采用该方法,可以设计聚束段腔间耦合孔的几何参数. 与实验结果的对照表明, 这是一种非常有效的非均匀加速结构腔间耦合孔设计方法.     

两腔高功率微波振荡器研究

对一种新型两腔振荡器进行了理论和数字模拟研究.这种结构中的调制腔实现电子束速度调制，调制后的电子束在通过两腔之间一个微波场较弱的区间时实现电子束群聚，然后在换能腔实现电子能量到微波能量的转换，并通过输出结构输出.同时，调制腔和换能腔之间存在微波耦合，换能腔中的一部分微波能量可以耦合到调制腔，形成一个正反馈回路，在一定条件下实行微波振荡.设计了一个X波段的器件，理论效率为294%，25维Particle in Cell(PIC)程序模拟的效率为28%，微波频率为942GHz，微波输出功率为225GW. 关键词： 高功率微波 微波腔 模式 自洽方程     

微片Ｎｄ∶ＹＡＧ 双频激光器腔调谐现象研究

 基于微片Ｎｄ∶ＹＡＧ 正交偏振双频激光器,研究了若干重要的双频激光器腔调谐现象, 包括光强调谐、频差调谐、子谐振腔效应及频差闭锁等,给出了实验结果和数据。腔调谐下,正交双频的频差调谐量约为３５０ ｋＨｚ;存在子谐振腔效应时,频差调谐量最大可达到２ ＭＨｚ;未发现明显频差闭锁现象,频差最小值可达到１４ ＭＨｚ。     

A novel design of Gaussian Wavelet Neural Networks for nonlinear Falkner-Skan systems in fluid dynamics

In this study, a design of integrated computational intelligent paradigm has been presented for numerical treatment of the one-dimensional boundary value problems represented with Falkner-Skan equations (FSE) by exploitation of Gaussian wavelet neural networks (GWNNs), genetic algorithms (GAs) and sequential quadratic programming (SQP), i.e., GWNN-GA-SQP. The GWNNs is used for mathematical modeling of the problem by constructing mean squared error based objective function while optimization of the cost function is initially conducted with efficacy of GAs as a global search and while fine tuning is performed with efficiency local search with SQP. The numerical results are obtained by proposed GWNN-GA-SQP for different FSEs arising in nonlinear regimes of computation fluid mechanics studies. A comparison of the results of proposed GWNN-GA-SQP stochastic numerical solver with reference state of the art solutions of Adams method establishes the accuracy, convergence and stability, which further endorsed through statistics on multiples runs. The T-Paired test is also applied to validate the effectiveness of the proposed GWNN-GA-SQP algorithm for solving nonlinear FSEs.     

Scattering by cavities of arbitrary shape in an infinite plate and associated vibration problems

This paper presents a solution for the displacement of a uniform elastic thin plate with an arbitrary cavity, modelled using the biharmonic plate equation. The problem is formulated as a system of boundary integral equations by factorizing the biharmonic equation, with the unknown boundary values expanded in terms of a Fourier series. At the edge of the cavity we consider free-edge, simply-supported and clamped boundary conditions. Methods to suppress ill-conditioning which occurs at certain frequencies are discussed, and the combined boundary integral equation method is implemented to control this problem. A connection is made between the problem of an infinite plate with an arbitrary cavity and the vibration problem of an arbitrarily shaped finite plate, using the jump discontinuity present in single-layer distributions at the boundary. The first few frequencies and modes of displacement are computed for circular and elliptic cavities, which provide a check on our numerics, and results for the displacement of an infinite plate are given for four specific cavity geometries and various boundary conditions.     

单片集成微环反射器可调谐半导体环形激光器理论和数值模型(英)

设计了一种新颖的快速可调谐激光器。这种激光器在恒定电流泵浦的有源微环组成的半导体环形激光器腔外部集成一个可调谐的无源微环反射器,其结构将决定激光器激射腔模的有源腔和无源可调谐部分分离,有助于提高调谐速度。与光栅结构的激光器相比,该激光器结构简单,具有强烈的选模功能,不需要相位匹配部分,输出波长不受调谐部分热效应的影响。基于多模速率方程建立了激光器的理论和数值模型,数值仿真结果表明该激光器能在选取的15个腔模范围内完成数字调谐,且具有40 mA的较低阈值电流和适中的边模抑制比。     

SOLUTION OF COUPLED ACOUSTIC PROBLEMS: A PARTIALLY OPENED CAVITY COUPLED WITH A MEMBRANE AND A SEMI-INFINITE EXTERIOR FIELD

There have been many attempts to understand the coupling phenomena between a solid structure and the surrounding fluid. However, the studies were restricted to interaction only between a structure and a finite cavity or a structure and acoustic field of infinite size. The system that we have studied has a structure that faces both a cavity of finite size and an external field of semi-infinite size. We also allow a hole, which can directly interact with the cavity as well as the external field. This configuration, therefore, provides two different interactions, or communication means. One is the finite structure and the other is the hole of finite size. This paper studies as to how these two components interact with the other two systems: the finite cavity covered by the structure and the hole, and the semi-infinite fluid. For simplicity, a two-dimensional and partially opened cavity coupled with a membrane and an exterior field was selected. The solution has to be found by solving a boundary value problem, but this case has to do with the boundaries that have two different conditions: one is the membrane and the other is the hole. The solution has been found in terms of the modal functions that satisfy the boundary conditions of finite cavity, membrane and hole. Non-dimensional coupling coefficients are obtained from the solution. The results exhibit that the coupling effect gives additional peaks and troughs in the averaged pressure of the cavity. These peaks and troughs are symmetrically arranged with respect to Helmholtz frequency of the cavity. The strong coupling occurs at the trough frequencies where the membrane interacts actively with the cavity and the exterior field.     

Tuning the Nigerian slit gong

An experimental and theoretical investigation of the Nigerian slit gong is reported. It is shown that in tuning the gong the artisan ensures that the frequencies of the two lowest mechanical resonances are nearly coincident with the frequencies of two of the acoustic resonances of the internal cavity. Four possible tuning parameters are identified and the effects of changing these parameters are discussed.     

Mode Suppression Phenomenon in a Mode Splitting He-Ne Laser

The mode competition is significant in laser physics and applications. A priority frequency will suppress, in competition, a potential frequency within gain profile, and this becomes more obvious with greatly decreasing the spacing of the two frequencies. The small spacing is produced by splitting one mode into two orthogonally polarized frequencies in a 0. 6328 μm He-Ne laser with a short cavity length (150 mm long). By tuning the cavity length, the intensities of the two frequencies (e-mode and o-mode) under a ariety of frequency spacings is measured. The suppression bandwidth for the potential mode is up to several hundreds of MHz and changes with the frequency spacing of the pair of frequencies. The intensities for the two frequencies are vary oppositely.     

Mode Suppression Phenomenon in a Mode Splitting He-Ne Laser

The mode competition is significant in laser physics and applications. A priority frequency will suppress, in competition, a potential frequency within gain profile, and this becomes more obvious with greatly decreasing the spacing of the two frequencies. The small spacing is produced by splitting one mode into two orthogonally polarized frequencies in a 0. 6328 μm He-Ne laser with a short cavity length (150 mm long). By tuning the cavity length, the intensities of the two frequencies (e-mode and o-mode) under a ariety of frequency spacings is measured. The suppression bandwidth for the potential mode is up to several hundreds of MHz and changes with the frequency spacing of the pair of frequencies. The intensities for the two frequencies are vary oppositely.