X波段加速管中高阶模电场分布的测试

介绍了一种用于测试X波段加速管中高阶模电场分布的笼子式微扰体的研制与标定.该微型扰动体通过专门设计加工的固定装置,在尼龙线表面平行沉积溅射数根金属丝膜制成.利用一标准圆柱腔,对笼子式扰动体的扰动因子进行了定标,证实金属丝笼子式扰动体与同外形尺寸的金属圆筒相比,具有高分辨率、高灵敏度的优点.采用笼子式扰动体测试了一根长30cm的X波段加速管中TM110模的纵向电场分布.     

X波段加速管加高阶模电场分布的测试

介绍了一种用于测试X波段加速管中高阶模电场分布的笼子式微扰体的研制与标定,该微型拢动体通过专门设计加工的固定装置,在尼龙线表面平行沉积溅射数根金属丝膜制成,利用一标准圆柱腔,对笼子式扰动体的扰动因子进行了定标,证实金属丝笼子式拢动体与同外形尺寸的金属圆筒相比,具有高分辨率、高灵敏度的优点,采用笼子式拢动体测试了一根长30cm的X波段加速管中TM110模的纵向电场分布。     

用拉盖尔-高斯激光对真空中电子直接加速

对用拉盖尔-高斯(LG)光束加速电子作了研究.结果表明，仅模指数为p和l=1的LG光束的纵向电场可用于加速电子.模指数为p和l=1的线偏振和圆偏振LG光束都对电子有加速效果.对轴上光场的相速度和群速度以及电子能量增益等物理特征作了讨论.给出了轴上光场的相速度和群速度、加速电位及电子能量增益等的解析表达式，并作了数值计算和分析. 关键词： 激光电子加速 拉盖尔-高斯光束 线偏振和圆偏振 能量增益     

驻波腔内电子运动过程的解析分析

考虑了加速电场的高次谐波的影响，解析地分析了电子在驻波腔内的运动过程，给出了电场分布，与数值模拟计算的电场分布比较吻合。讨论了高次谐波对电子束横向运动的影响，利用此解析解可选择高亮度注入器腔的最优电场分布。并得出射频驻波腔内电子束在β趋于１时射频场效应趋于零的结论。     

静电加速管中强流空间电荷效应的研究

 对一种工业用大功率电子加速器(450kW)的加速管中的空间电荷效应作了5点假设，建立了物理模型。对模型的束内外径向电位分布、空间电荷对轴上电位的影响，以及空间电荷力对束流传输的影响等进行了理论分析，得到了束内径向电位分布。结果表明：束流内部径向电位沿径向均呈抛物线变化，并在轴上达到最小值；而空间电荷产生的束内电场与半径呈线性变化；空间电荷不仅会引起轴上电位的跌落，而且对束流有发散作用，特别是在电子速度较低时更为明显。在考虑了空间电荷效应后，强流静电加速管的电场设计关键在加速管的前端，与弱流加速管相比，强流加速管的电场变化要大得多。     

驻波加速管中的电子反轰现象

在以半腔为首腔的边耦合驻波加速管中观察到了电子反轰现象,由于电子反轰的结果,导致电于枪发射电流非正常增长。本文从纵向运动方程出发,用相轨道方法分析了驻波加速管中的电子反轰运动,并计算了不同电场分布、不同电场幅值及不同注入电压对电子反轰的影响。     

1+1/2 Cell超导加速腔的本征高阶模场分布研究

为实现高平均流强加速, 需要有效地消除超导加速腔中的高阶模场. 为研制有效的高阶模耦合器, 本文对北京大学DC-SC光阴极超导注入器的核心部件—1+1/2 cell超导加速腔中高阶模场进行了分析研究, 用HFSS程序计算给出前31个高阶模场参数, 与实验测量较为符合. HFSS计算与Superfish计算结果比较符合很好, 验证用HFSS计算可靠, 为以后超导腔的升级研究提供有效的手段.     

TESLA式高阶模衰减器的改进与设计研究

为了消除超导加速腔中高阶模场对加速粒子的影响, 在DESY的高阶模耦合器结构的基础上本文提出了改进的耦合器. 用HFSS程序针对1.5cell腔设计优化了高阶模耦合器, 得到高阶模耦合器对几种主要模式的吸收. 研究结果表明, 采用新型结构后, 衰减器对主要有害模的衰减由－40dB提高到－15dB, 使原有高阶模衰减器的性能明显提高. 该高阶模衰减器也适用于国产2cell超导腔的使用.     

增益波导垂直腔面发射激光器中的模式分析及实验研究

本文研究了增益波导垂直腔面发射激光器的横向及纵向模式特性。采用二维延伸抛物型复折射率波导结构从理论上分析了增益波导垂直腔面发射激光器中模式的横向电场分布、模式间隔、模式增益对远场分布图和光束发射角、耦合效率等.实验中在阈值电流之上既观测到稳定的基模工作,也观测到高阶非简并模工作等不同的光谱结构及远场分布,理论和实验基本吻合.     

非傍轴LG_(00)模与LG_(10)模高斯光束的远场分布特性

基于扁椭球面坐标系下非傍轴高斯光束的电场分布表达式,给出非傍轴LG_(10)模高斯光束的远场电场振幅分布表达式;分析了非傍轴LG_(00)模和LG_(10)模高斯光束的远场电场振幅分布特性;计算了非傍轴与傍轴高斯光束远场电场振幅分布的匹配效率和二阶矩参量的相对计算误差。分析表明,当扁椭球坐标系的半焦距远大于波长时,非傍轴LG_(00)模和LG_(10)模高斯光束的远场电场振幅分布趋近于傍轴LG_(00)模和LG_(10)模高斯光束的远场电场振幅分布。     

Study on the RF performance of 2-cell superconducting cavity

The physical design of the 2-cell superconducting cavity is presented. The RF parameters of the cavity and HOMs （high order modes） are reported. In this paper, we put the emphasis on the analysis of the HOMs and interaction between beam and cavity.     

Study on the RF performance of 2-cell superconducting cavity

The physical design of the 2-cell superconducting cavity is presented.The RF parameters of the cavity and HOMs (high order modes) are reported.In this paper,we put the emphasis on the analysis of the HOMs and interaction between beam and cavity.     

Measuring the performance of the coaxial HOM coupler on a 2-cell TESLA-shape copper cavity

Coaxial High Order Mode （HOM） couplers have been fabricated at Peking University and their RF performance has been measured on a test device consisting of a coaxial transmission line and a 2-cell TESLA-shape copper cavity. The test results on the 2-cell TESLA-shape copper cavity with HOM couplers indicate that the coupler can cut off the fundamental mode TM010 and absorb HOMs effectively after a careful adjustment. The optimal angle of the HOM coupler with the beam tube is found. The initial test results of HOM couplers are presented in this paper.     

RF characters study of a pick-up parallel-setting HOM coupler

A pick-up parallel-setting high order mode coupler(pps-HOM coupler)has been fabricated at Peking University.It has been tested on a coaxial transmission line and a 2-cell TESLA-shape copper cavity.The test result of the 2-cell TESLA cavity shows that the coupler can cut off the fundamental mode TM010 and absorb HOMs electively.As its RF properties are insensitive to the probe dip length,there is no need to adjust the probe repeatedly during practical operation.     

Measuring the performance of the coaxial HOM coupler on a 2-cell TESLA-shape copper cavity

Coaxial High Order Mode (HOM) couplers have been fabricated at Peking University and their RF performance has been measured on a test device consisting of a coaxial transmission line and a 2-cellTESLA-shape copper cavity. The test results on the 2-cell TESLA-shape copper cavity with HOM couplers indicate that the coupler can cut off the fundamental mode TM010 and absorb HOMs effectively after a careful adjustment. The optimal angle of the HOM coupler with the beam tube is found. The initial test results of HOM couplers are presented in this paper.     

Study on the HOMs coupler design of spoke cavity

The superconducting spoke cavity has been proposed to accelerate the proton in the low energy section of high power proton linac for an Accelerator Driven Sub-critical System (ADS).Considering that the High Order Modes (HOMs)in the superconducting cavity have far reaching influence on power dissipation and beam stability,the analysis of HOMs of the spoke cavity is needed.In this paper,we put emphasis on the analysis of HOMs of the spoke cavity and the HOMs coupler design.     

HOMs simulation and measurement results of IHEP02 cavity

In accelerator RF cavities, there exists not only the fundamental mode which is used to accelerate the beam, but also higher order modes(HOMs). The higher order modes excited by the beam can seriously affect beam quality, especially for the higher R/Q modes. 1.3 GHz low-loss 9-cell superconducting cavity as a candidate for ILC high gradient cavity, the properties of higher order mode has not been studied carefully. IHEP based on existing low loss cavity, designed and developed a large grain size 1.3 GHz low-loss 9-cell superconducting cavity(IHEP02cavity). The higher order mode coupler of IHEP02 used TESLA coupler's design. As a result of the limitation of the mechanical design, the distance between higher order mode coupler and end cell is larger than TESLA cavity.This paper reports on measured results of higher order modes in the IHEP02 1.3 GHz low-loss 9-cell superconducting cavity. Using different methods, Q e of the dangerous modes passbands have been obtained. The results are compared with TESLA cavity results. R/Q of the first three passbands have also been obtained by simulation and compared with the results of the TESLA cavity.