First experimental research of the bunch compressor at CAEPLI

Magnetic bunch compressor is one of the key technologies on the path to next generation accelerator driven facilities. In this paper we report the design principles and the first experimental research of the bunch compressor developed at Chinese Academy of Engineering Physics (CAEP). The length of the bunch after compressor is found to be about 0.7 ps (rms) and the peak current exceeds 500 A when operated in the optimized condition. The sensitivity of the bunch length on the phase of the acceleration field and magnetic field of the bunch compressor was also measured and analyzed.     

束团磁压缩的高阶限制

研究了束团压缩中的高阶效应, 结果表明存在高阶项的压缩限制, 压缩后束团的长度比线性理论值长, 初始为均匀分布的束团较高斯分布更易压缩, 在相同的加速段与磁压缩器条件下, 其所获得的束团长度较短, 最后作了数值计算, 结果与理论相符.     

合肥光源单束团下束团长度和能散的测量

根据同步光与储存环中的束流信号具有相同的时间结构的原理,测量同步光脉冲的半高全宽值可以计算出束团的长度。根据合肥光源的特点和实际需要,选择快速光电接收器搭配高速高带宽示波器作为在线测量束团长度和纵向分布等的主要手段。对单束团模式下束团长度随流强和高频腔腔压的变化趋势进行了测量。测量结果表明：束团长度与腔压的0.3次方成反比,比理论值0.5小;而束团长度随流强的增长率为2.0 ps/mA。通过测量纵向量子寿命进行了能散随流强变化的间接测量,结果表明,束团的拉伸是能散变化和势阱效应共同作用的结果。     

磁压缩对高频稳定性的要求

曲柄式磁压缩系统是北京大学SASE自由电子激光装置中非常重要的部分,通过其对电子束团的压缩为扭摆器提供高流强、短脉冲的电子束,使电子束在扭摆器内较短的距离实现饱和出光。曲柄式磁压缩需要利用偏离高频峰位的加速相位使得电子束产生能量-位置关联,主要讨论高频相位抖动与能量-位置关联的相互关系,高频相位抖动使得束团的能量-位置关联不同,即束团内电子能量随位置分布不同。进而研究其对磁压缩性能的影响,即能量-位置关联不一样会导致磁压缩得到的束团长度出现涨落。     

磁压缩对高频稳定性的要求

 曲柄式磁压缩系统是北京大学SASE自由电子激光装置中非常重要的部分,通过其对电子束团的压缩为扭摆器提供高流强、短脉冲的电子束,使电子束在扭摆器内较短的距离实现饱和出光。曲柄式磁压缩需要利用偏离高频峰位的加速相位使得电子束产生能量-位置关联,主要讨论高频相位抖动与能量-位置关联的相互关系,高频相位抖动使得束团的能量-位置关联不同,即束团内电子能量随位置分布不同。进而研究其对磁压缩性能的影响,即能量-位置关联不一样会导致磁压缩得到的束团长度出现涨落。     

CTF磁压缩器的误差研究

磁压缩器广泛应用在自由电子激光装置中. 电子束团的归一化发射度增长由二极磁铁的高阶分量误差及准直误差引起. 本文描述了CTF (CXFEL Test Facility)的第一个磁压缩器的误差研究.     

Study on ILC bunch compressor

In this paper, we have found a new set of parameters for the short two-stage     

Study on ILC bunch compressor

In this paper, we have found a new set of parameters for the short two-stage ILC bunch compres-sors. The RF sections are both in the accelerating phase rather than the decelerating phase to improve the accelerating efficiency. We have also studied the CSR related issues. The results show that the microbunch instability exists extensively in the second bunch compressor, but the emittance dilution is small due to the relatively long bunch.     

束团压缩用踢波器的模型腔

 为了提高中子产额,法兰克福强中子源采用Mobley型束团压缩器来增强打靶时质子流的密度,其入口处由射频踢波器实现微脉冲的偏转,踢波器由一对电偏转板和串联电感线圈组成谐振腔体。考虑到高频下寄生电容效应、导体腔壁对线圈电感的影响以及涡流效应对线圈交流电阻的影响,对一台模型腔的射频特性进行了理论预测。对腔体内电磁场分布进行了数值模拟,并利用电容微扰法进行了冷模测量。针对谐振频率、品质因数和并联分路阻抗等参数,分析比较了理论计算、数值模拟及冷模测量的结果,总结得出射频踢波器的有效设计方法。     

束团压缩用踢波器的模型腔

为了提高中子产额,法兰克福强中子源采用Mobley型束团压缩器来增强打靶时质子流的密度,其入口处由射频踢波器实现微脉冲的偏转,踢波器由一对电偏转板和串联电感线圈组成谐振腔体。考虑到高频下寄生电容效应、导体腔壁对线圈电感的影响以及涡流效应对线圈交流电阻的影响,对一台模型腔的射频特性进行了理论预测。对腔体内电磁场分布进行了数值模拟,并利用电容微扰法进行了冷模测量。针对谐振频率、品质因数和并联分路阻抗等参数,分析比较了理论计算、数值模拟及冷模测量的结果,总结得出射频踢波器的有效设计方法。     

单谐振腔束团长度监测器的设计与仿真

提出了一种利用单个谐振腔测量直线加速器束团长度的新方法。不同于传统的双谐振腔束团长度监测器,该方法仅需要使用单个谐振腔,省去了用于辅助测量的参考腔,从而简化了装置结构,节省了空间。针对国家同步辐射实验室基于可调谐红外激光的能源化学研究大型实验装置进行了监测器的物理设计。通过设定同轴探针的插入位置,解决了双模信号互相干扰的问题,利用微扰金属改变调节工作频率,克服了双模难以同时谐振的困难。利用CST软件进行建模和仿真。仿真结果表明,该监测器可实现2～5 ps束团长度的诊断,测量误差小于5%。     

基于束流位置探测器的束团长度测量

分析了驱动电子束团的频域特性,研究了基于该特性进行长度测量的理论基础;使用三维模拟软件对束流位置探测器(BPM)进行建模,用模拟的方法对传输阻抗进行了数值计算;对不同长度的束团进行了测量和计算,并且分析了束团位置在真空管道中偏移对束团长度测量的影响。由测量结果可见,电子束团长度在10~100 ps(3~30 mm)时,测量误差均小于2%,满足中国工程物理研究院高平均功率自由电子激光太赫兹实验测量的使用要求。     

基于束流位置探测器的束团长度测量

分析了驱动电子束团的频域特性,研究了基于该特性进行长度测量的理论基础;使用三维模拟软件对束流位置探测器(BPM)进行建模,用模拟的方法对传输阻抗进行了数值计算;对不同长度的束团进行了测量和计算,并且分析了束团位置在真空管道中偏移对束团长度测量的影响。由测量结果可见,电子束团长度在10~100 ps(3~30 mm)时,测量误差均小于2%,满足中国工程物理研究院高平均功率自由电子激光太赫兹实验测量的使用要求。     

Generation and measurement of sub-picosecond electron bunch in photocathode rf gun

We consider a scheme to generate a sub-picosecond electron bunch in the photocathode rf gun by im-proving the acceleration gradient in the gun, suitably tuning the bunch charge, the laser spot size and the acceleration phase, and reducing the growth of transverse emittance by laser shaping. A nondestructive technique is also reported to measure the electron bunch length, by measuring the high-frequency spectrum of wakefield radiation which is caused by the passage of a relativistic electron bunch through a channel surrounded by a dielectric.     

负动量压缩因子磁聚焦结构在τ–粲工厂储存环设计中的应用

研究并提出了一个负动量压缩因子(α_p<0)τ–粲工厂储存环磁聚焦结构.对其束团拉伸的计算表明:在设计流强,束团长度将比自然束长短,束团长度不会拉伸.     

Electro-optical sampling non-synchronous delay scanning measurement of electron beam bunch length at BFEL

The Electro-optical sampling delay scanning technique can be used for electron beam bunch length measurement.A novel non-synchronous delay scanning technique based on the electro-optical sampling measurements is presented.Based on Beijing Free Electron Laser(BFEL),the electron beam bunch length was measured with the electro-optical sampling technique for the first time in China.The result shows that the electron beam bunch length at BFEL is about 5.6±1.2 ps.     

TM020模式谐振腔束团长度监测器的设计与仿真（英）

提出了一种基于高次模式的谐振腔束团长度测量技术,新方法的谐振腔工作于高次本征模式TM0n0。这样的谐振腔拥有更大的腔体半径,从而移除了谐振腔半径必须大于束流管道半径这一原则带来的工作频率限制。为国家同步辐射实验室未来的正电子源设计了一台双腔束团长度监测器,讨论了谐振腔工作频率的选择并推导了束团长度的计算公式,监测器的谐振腔工作于TM020模式,其半径远大于使用TM010模式的传统方法,在CST软件中模拟的结果显示其束团长度测量精度好于7%。     

Calculations for shortening the bunch length in storage rings using a harmonic cavity

Using the Hefei Light Source phase Ⅱ project （HLS- Ⅱ） as an example, a theoretical analysis of shortening the bunch lengths using a higher harmonic cavity （HHC） is given. The threshold voltage of an active HHC and the threshold tuning angle of a passive HHC are first analysed. The optimum tuning angle for the constant detuning scenario and the optimum harmonic voltage for the constant voltage scenario are presented. The calculated results show that the reduced bunch length is about half that of the nominal bunch. The bunch lengths vary from 11 mm at 0.1 A to 7 mm at 0.4 A for the constant detuning scenario, while the bunch lengths are around 7 mm over the beam current range for the constant voltage scenario. In addition, the synchrotron frequency spread is increased. It indicates that HHC may be used to reduce the bunch length and increase the Landau damping of synchrotron oscillations in a storage ring.     

皮秒量级电子脉冲宽度测量系统

提出了一种测量皮秒量级电子脉冲宽度的新方法; 并且在二次发射微波电子枪前期研究结果的基础上利用MAFIA等数值模拟程序建立起该测量方法的数值模型进行数值分析, 讨论了其可行性; 并根据本实验室现有条件给出了测量方法的最小分辨, 说明了测量方法的可行性.     

Bunch length measurement using a traveling wave RF deflector

RF deflectors can be used for bunch length measurement with high resolution. This paper describes a completed S-band traveling wave RF deflector and the bunch length measurement of the electron beam produced by the photocathode RF gun of the Shanghai DUV-FEL facility. This is the first time that such a transverse RF deflector has been developed and used to measure the bunch length of picosecond order in China. The deflector's VSWR is 1.06, the whole attenuation 0.5 dB, and the bandwidth 4.77 MHz for VSWR less than 1.1. With a laser pulse width of 8.5 ps, beam energy of 4.2 MeV, and bunch charge of 0.64 nC, the bunch lengths for different RF input power into the deflector were measured, and an averaged rms bunch length of 5.25 ps was obtained. A YAG crystal is used as a screen downstream of the deflector, with the calibrated value of 1 pix = 136 μm.