光控介质谐振器振荡器的实验研究

本文报道了关于光控介质谐振器振荡器的实验结果。对一只9.5GHz的介质谐振器振荡器进行实验,用硅半导体光敏材料,入射15mW红光,光控频率调谐达17.5MHz,红光功率的平均频率调谐率为1.17MHz/mW。入射5.5mW紫光,光控频率调谐达到12.3MHz,紫光功率的平均频率调谐率为2.24MHz/mW。在整个调谐范围内振荡器的微波输出功率随光功率增加而略有上升。     

微波谐振腔Q值对磁激子振幅不稳定态阈值的影响

基于Safonov和Yamazaki所发展的激励自旋波非线性辐射衰减的理论［J. MMM. 161 (1996 ) 275］, 考虑磁激子与磁激子以及磁激子与光子的两种非线性相互作用过程，计算了微波谐振腔Q值对磁激子振幅不稳定态阈值的影响，结果与实验数据基本一致. 关键词： 磁激子 谐振器 铁磁体     

聚心火焰在共振腔作用下引发爆轰的数值研究

 基于带化学反应的二维轴对称Euler方程，利用带有Superbee限制函数的波传播算法，对共振腔中的氢气-空气预混气的聚心燃烧进行了数值模拟，讨论了共振腔不同抛物面对起爆的影响。数值结果表明，在开始阶段，燃烧诱导的激波在轴心、火焰和固壁的反射，使火焰失稳，随后共振腔中的抛物壁面上产生一定频率和强度的反射激波，不断穿越火焰，使火焰进一步失稳，加剧了燃烧速度，最终导致爆轰的形成。同时，火焰在与激波的作用过程中，形状扭曲变形，呈封闭端小敞口端大的扁平头部蘑菇云。共振腔抛物面的不同形状引起激波聚焦位置的变化，会影响激波和火焰的相互作用，使起爆提前或推迟，甚至不起爆。     

片式多层陶瓷微波谐振器

介绍了片式陶瓷微波谐振器的工艺过程、谐振器的结构以及结构对谐振器参数的影响,谐振器与外电路的耦合采用耦合间隙的方法与谐振单元在同一层内实现,这种新结构既可给制备工艺带来方便,又可减少工艺所带来的误差。用多层陶瓷工艺技术,用高介电常数、低温烧结微波陶瓷实现了中心频率为1GHz,有载品质因数大于80的试验双端口多层微波谐振器。微波谐振器体积小,整个谐振器的尺寸为7mm×2mm×1mm,适用于表面贴装技术。     

TE011模高功率窄带带通滤波器设计

利用圆腔ＴＥ０１１模的高Ｑ值特性，设计了高直接耦合式窄带带通滤波器，并给出了具体的设计步骤和实例，理论与实验结果基本一致。     

HL-2A装置快速扫描气动探针的研制和运用

快速扫描气动探针已在HL- 2A 装置上用于对边缘等离子体参数的径向分布的测量, 特别是刮离层等离子体参数的特征长度和扰动的测量。该系统采用精密的气动气缸驱动带有探针组件的长驱动杆, 其最快速度可在60 ms 时间内水平扫描8 cm 的距离。探针信号测量具有1MHz 的快速时间响应和0. 04 mm 的空间分辨率。可靠地测量了HL- 2A 装置边缘电子温度和密度的时空分布。     

Improvement of the spinning electrophorometer for zeta potential measurements

In this study, bubbles are held by centripetal force at the center of a rotating cylinder filled with an aqueous solution. Their velocities along the axe of rotation, after application of an electrophoretic force, are used for the calculation of the so-called electrokinetic potential. But this process necessitates the elimination of the electro-osmosis which occurs on the interior sides of the glass cylinder by superposing a concurrent force on the bubble. Efficiency of DEAE-Dextran reticulated with 1,4 Butanediol Diglycidyl Ether can be tested by the observation of a cloud of latex microspheres injected in the interior of the tube and allowed to move in respect with the application of an electric field. The experimental control of these velocity profiles proves the adequacy of the polymer for many cases such as surfactant solutions, presence of electrolytes, utilization with moderate pH.The dynamic interpretation of the electrophoretic motion of bubbles is possible by considering that small ones behave like rigid spheres moving in a rotating fluid. In the second part of this paper and in a previous publication, we have experimentally proved that the use of the theoretical expressions of the forces involved for rigid spheres is justified for small bubbles. So, the electrokinetic potential can be expressed versus the velocity, leading to possible interpretations of the adsorption on gas-water interfaces.     

一种新型L波段带通滤波器的设计

本文给出了一种具有平行耦合线分裂环谐振器式Ｌ波段带通滤波器的近似设计方法及实验结果。这种滤波器结构简单，宜用于微波单片集成电路。     

Poloidal–toroidal decomposition in a finite cylinder. I: Influence matrices for the magnetohydrodynamic equations

The Navier–Stokes equations and magnetohydrodynamics equations are written in terms of poloidal and toroidal potentials in a finite cylinder. This formulation insures that the velocity and magnetic fields are divergence-free by construction, but leads to systems of partial differential equations of higher order, whose boundary conditions are coupled. The influence matrix technique is used to transform these systems into decoupled parabolic and elliptic problems. The magnetic field in the induction equation is matched to that in an exterior vacuum by means of the Dirichlet-to-Neumann mapping, thus eliminating the need to discretize the exterior. The influence matrix is scaled in order to attain an acceptable condition number.     

Aperture array Fabry-Perot interference filter

We demonstrate effective implementation of the Fabry-Perot interferometer with subwavelength aperture arrays on its two metal mirrors to achieve polarization-independent narrow band-pass filtering. By superimposing of aperture array fundamental resonance transmission with one of the Fabry-Perot interference peaks, the moderate filter insertion loss of −5 dB, narrow band-pass width of 15 μm, and efficient out-of-band rejection within the ∼0.1-3 THz range are reported. The Siemens-star-shaped apertures in arrays play an important role to achieve such polarization independence and small insertion loss.