静电偏转型摄像管聚焦偏转系统设计Ⅰ-场的计算

磁聚焦静电偏转(MS)和静电聚焦静电偏转(SS)型摄像管具有图像失真小,分辨率高且均匀,电子束易于垂直上靶,阴影小等优点,所以受到人们的重视。但图案偏转电极的形状复杂,非对称场的计算较困难。本文对静电偏转型聚焦偏转系统的结构作了分析研究,远用分离变量法给出了圆柱坐标中静电聚焦(旋转对称)场和静电偏转(非旋转对称)场的解析解,并给出了计算实例。     

附加电极对扫描变像管性能的优化

 通过分析影响变像管性能的主要因素,以提高其时间分辨率、空间分辨率和动态范围为优化思路,确定了在扫描变像管中荧光屏邻近区域引入等径螺旋电极以产生纵向均匀加速场的优化方案。分析得知,该优化结构可以在几方面改善变像管的性能:增加粒子到达荧光屏的纵向速度、减小粒子通过偏转板与荧光屏之间区域的渡越时间和渡越时间弥散、提高荧光屏的亮度。在横向约束带电粒子束的发散,通过减小空间电荷像差而改善电子光学系统的空间分辨率。另外,附加电极的引入也为降低加速阳极电位和偏转电极电位从而提高偏转系统的灵敏度提供了一定的空间。     

行波偏转器前置短磁聚焦条纹变像管理论设计与实验研究

条纹变像管因其超高时间分辨特性而成为实现皮秒至飞秒量级时间分辨的重要测量仪器.本文设计了一种同时兼顾高时空分辨的行波偏转器前置短磁聚焦条纹变像管.该管型通过减小电子渡越时间以抑制空间电荷效应、采用偏转器前置以及行波偏转方式提高偏转灵敏度,实现整管时空分辨率的大幅提升.利用CST微波工作室有限元法数值计算条纹变像管行波偏转器的通频带宽、偏转灵敏度,结果表明:本设计中的行波偏转器因其较高的通频带宽特性实现了偏转器上的电磁波相速度在很宽频率范围内与电子轴向群速度匹配,产生更有效偏转.利用CST粒子工作室模拟追踪光电子的运行轨迹,通过最佳像面上的时间调制传递函数和空间调制传递函数,计算得到其理论时间分辨率可达220 fs,空间分辨率高于100 lp/mm.同时根据像差定义给出追踪实际电子轨迹的像差计算方法,实现对变像管成像质量评价.最后利用紫外灯对其进行静态测试,获得静态空间分辨率优于35 lp/mm的结果.     

������ע������ƫתϵͳ�IJ������������о�

为EAST装置中性束注入器设计了一套用于将剩余离子在线电偏转的结构,并对系统各设备的核心参数进行了估算。在4.41kV偏转电压作用下,该电偏转系统可提供80keV氘离子束偏转所需的偏转电场。在偏转电场调制情况下,该电偏转系统可有效降低极板表面的热负荷,进而满足EAST中性束注入器稳态运行的需要。     

中性束注入器电偏转系统的参数设计与估算研究

为EAST 装置中性束注入器设计了一套用于将剩余离子在线电偏转的结构,并对系统各设备的核心参数进行了估算。在4.41kV 偏转电压作用下,该电偏转系统可提供80keV 氘离子束偏转所需的偏转电场。在偏转电场调制情况下,该电偏转系统可有效降低极板表面的热负荷,进而满足EAST 中性束注入器稳态运行的需要。     

介绍一种新型的电子束场偏转演示实验装置

新型的电子束场偏转演示实验装置,由特制的电子束旋偏管和高压电源组成。它介于场效应阴极射线管和荷质比演示实验装置之间,主要用于演示运动的带电粒子在外场中受外场力作用而发生偏转,见图1.偏转的方向由外场的方向决定。     

一种8行任意扫描的电光扫瞄器

 针对激光的快速智能扫描,综合利用晶体的双折射效应和电光效应,提出一种电控集成8行任意扫瞄的高速光扫描方案。主要由三级数字电光偏转器和8×1的周期性极化电光棱镜组构成,其中3个电光快门和3块双折射晶体构成三级数字偏转器,通过半波电压的控制实现行位置的转换,一定数目的周期性极化电光棱镜级联组成单行偏转器,通过控制电压进行单行扫描,根据电场施加方式可实现数字型或者连续型扫描。利用梯形结构的电光棱镜组设计了最大电压为5.822 kV时,扫描视场为17.256°的可通过联机控制进行任意行扫描的高速激光扫描器。     

HL-2M装置5MW-NBI加热束线偏转磁体研制

根据HL-2M装置5MW-NBI加热束线总体设计参数、注入器的部件空间布局、几何汇聚特点等,建立了基于8饼线圈的注入器偏转磁体3D模型。利用电磁场模拟软件CST Studio详细模拟了注入器的偏转磁体产生的偏转磁场分布,不同成份离子束的偏转轨迹。在模拟分析结果的基础上优化了偏转磁体的物理结构,完成了磁体的工程设计、加工和测试。偏转磁体的磁场测试结果表明,测试值与CST计算值的偏差小于±5%,达到注入器偏转磁体设计要求。     

衍射现象对高精度偏转器设计的影响

基于波动光学理论,计算了由衍射、球差和色差三者共同作用的电子束斑电流分布,得到了电子束斑的精确信息和电子束曝光机的轴上分辨率。针对某一个具体系统的不同电子束孔径角,以偏转器的位置和相互转角为变量进行了偏转系统的优化设计;综合考虑了电子光学系统的衍射、轴上像差和偏转像差三者与光阑孔径角的不同关系。得到了光柱体的最佳总体性能,保证了电子束曝光机的高分辨率和均匀性。     

新型KTP电光偏转器的设计和分析

设计了新ＫＴＰ电光偏转器，当通光口径Ｄ＝４ｍｍ，长度Ｌ＝４０ｍｍ时，其时间分辨率为１８０ｐｓ，从而可获得最窄宽度为４００ｐｓ的整形激光脉冲，而相同结构的ＬｉＮｂＯ３电光偏转器最窄只可获得宽度为８３０ｐｓ的整形激光脉冲，分析了电光偏转器设计中影响其性能指标的因素，指出利用恒温炉装置可消除激光脉冲在传播过程中的波面畸变。     

Ion-optical system with energy filtering for a monopole mass spectrometer

An electrostatic ion-optical system providing angular focusing of the beam and its monochromatization at the entrance to a monopole mass spectrometer is suggested and analyzed. The system uses a funnelshaped extracting electrode and a cylindrical energy filter with a flat electrode in its meridional plane. The geometry of the system and the supply voltage can be varied in proportion to the aperture radius and anode potential, respectively.     

一种条纹变像管静态电子光学聚焦特性数值模拟

 对ICF实验中条纹相机的重要组件变像管的工作过程进行了介绍,建立了其内部电子光学系统模型,对其静态电子光学特性进行了数值模拟。模拟软件采用ANSYS,数值计算基于有限元数值计算方法,并利用哈密顿原理求解泛函,在控制计算精度的基础上,得出了该电子光学系统的内部静电场分布和轴上电位分布,同时对静态条件下的电子轨迹进行了模拟计算。结果显示了与理论解析结果很好的相似性,同时初步探索了电极尺寸及电压参数对成像的影响。结果表明,电压参数的改变对光电子成像的影响要更大一些。     

大动态范围软X射线飞秒变像管

 为获得能够实际应用的飞秒时间分辨软X射线变像管,提出并完成了一种新的扫描变像管管型的理论设计。新管型采用五电极平面对称静电柱透镜,它易于对电子束进行强聚焦,且没有轴对称透镜的电子束聚焦交叉点,由此可以缩短变像管长度,减小渡越时间弥散和抑制空间电荷效应,从而提高动态范围和时间分辨率。通过模拟计算得到：在光电子初能量色散半高宽为1.6 eV、狭缝面积为10 mm×20 μm、时间分辨能力为500 fs时,软X射线变像管有用的动态范围约100倍。     

New electrostatic cylindrical energy analyzer

The focusing properties of an ideal cylindrical field in full relativistic field have been investigated for charged particles originating from an extended source and an analytical solution for the equations of motion has been provided. This focusing system can be used for production of electrostatic energy analyzer provided surface analysis from an extended area.     

Electrostatic force acting on conductive ball between electrodes II: Cylindrical upper electrode with hemispherical tip for capturing/releasing conductive ball

The electrostatic force between a conductive ball on a plane electrode and a cylindrical electrode with a hemispherical tip is analyzed. A cylindrical electrode with a dielectric film for realizing a new LSI bonding system is proposed. The force on the ball increases with increasing diameter of the cylindrical electrode. When a dielectric film is placed under the cylindrical upper electrode with a fixed gap between the electrodes, the force acting on the ball increases with increasing dielectric film thickness. Capture of the ball was experimentally confirmed. This study provides a useful foundation for electrostatic manipulation of a conductive ball.     

A mathematical model of external electrostatic field of a special collector for electrospinning of nanofibers

This article focuses on the analysis of electrostatic field generated by a special collector consisting of two parallel cylindrical conductors used for electrospinning. Computed values of critical electrical potential obtained by an analytical model are compared with measurements. Here we show that the gap distance between the special collector and a spinning electrode, i.e., a syringe needle, has not substantial effect on the critical potential if the special collector distance from the syringe needle is higher than the gap distance between cylindrical conductors. The presented model is a good analytical approximation of electric field created by the used special collector.     

变像管皮秒分幅和飞秒扫描相机的实验研究

本文将描述两种变像管皮秒分幅相机和一种飞秒扫描相机的设计特点、动态测试方法和实验结果。第一种变像管皮秒分幅相机采用了交叉点扫描多光栏分幅的方法,其变像管具有长加速电极和短阳极的静电弱聚焦系统与偏转灵敏度高、偏转像质好的偏转群体结构;其超快速控制电路只需一个光电开关斜坡电压脉冲发生器和一个特殊设计的脉冲成形网络即可送出具有合适时间关联的4对正负极性三角波和一对正负极性的单台阶液电压脉冲。实验表明,该相机在提供6幅分幅图像的情况下,每幅图像全曝光时间为80ps,除 3～4幅图像间的时间间隔为680ps外,其余均为160ps,动态空间分辨率达到5.51p/mm。第二种变像管皮秒分幅相机采用快门式分幅方法;其变像管采用行波偏转系统,内增强MCP做成带状线结构,并具有输入输出阻抗变换器,其三台阶波和快门脉冲序列均由光电开关电路和脉冲成形网络产生。该相机在提供三幅分幅图像的情况下,每幅图像全曝光时间为660ps,画幅之间的时间间隔均为4ns,动态空间分辨率为5.5lp/mm。飞秒扫描相机采用MCP内增强飞秒扫描变像管、具有负时间畸变的中继透镜和无触发晃动的光电开关扫描电路。实验证明,该相机在时间分辨率为500fs时,其动态范围为30;当时间分辨率为1.2ps时,其动态范围可达500;无扫描图像弯曲现象,触发晃动为±2ps.     

Computer analysis of the source image structure in 3D electron-optic systems: I. An electrostatic system

Computer analysis of the arbitrary source image obtained in 3D electron-optic systems is performed. The systems involve electrostatic fields focusing and deflecting electron beams. Specifically, the structure of a net electron beam from an extended source at the crossover is examined. It is shown that the spread function of the source, which characterizes the imaging quality of the system most fully, may serve as a primary computational criterion.     

Cone electrostatic energy analyser of high luminosity

It is proved that the conical electrostatic potential Φ=−ln(tg(γ/2)) is the only axisymmetric Laplace potential which depends only on γ—the angular coordinate of the cylindrical coordinate system (z,r,γ). It is also shown that, thanks to the meridional beam broadening which is inherent in Φ, the analyser based on such a potential can have a resolution several times better than that of the well-known 42.3° cylindrical mirror analyser (CMA), their luminocities being equal. The main electron-optical parameters of the hypothetical analysers based on the potential Φ are described in detail in the case of the narrow inner field-forming electrode. This case is considered to be interesting in electron spectroscopy practice.     

Numerical study on electrostatic potential distribution of large cylindrical oil tanks

This study carried out a numerical simulation of electrostatic potential distribution in the cylindrical oil tank, focusing on spatial distribution of electrostatic potential and the variation tendency of the potential in the filling operation. Electrostatic potential distribution of stationary oil was illustrated, and the relationship between the electrostatic potential distribution and some parameters of the tank and oil was analyzed as well. Dynamic electrostatic distribution was studied when charged oil is filling into the tank, and ESD prevention measures’ effects on electrostatic potential distribution were simulated. Finally, calculation results of two other types of oil tanks were presented in brief.