冷却储存环CSRm中螺线管场耦合效应研究

介绍了重离子冷却储存环中螺线管场对束流水平方向和垂直方向产生耦合的原理, 由耦合运动方程及耦合系数推导出螺线管场耦合的补偿方法. 结合兰州冷却环主环实际的单元结构,工作点选在束流稳定的差共振附近, 模拟计算了冷却环主环在电子冷却段没有螺线管、有螺线管和增加补偿螺线管三种情况下的束流发射度及此三种情况下冷却环主环的动力学孔径. 通过模拟计算可知螺线管的存在将引起束流的水平方向和垂直方向严重耦合, 由于耦合效应, 垂直方向的发射度将超出其接受度, 致使束流大量损失. 针对这种情况, 提出了在螺线管两端的合适位置增加一组补偿螺线管的校正方案. 模拟结果表明这种措施行之有效.     

CSRm束流径向和轴向振荡的耦合

 介绍了由于磁铁的安装误差和螺线管的存在而造成的束流径向和轴向的耦合，以及耦合对束流稳定的影响。结合CSRm结构的典型参数分析得出：二极磁铁和四极磁铁在纵向角安装偏差为-0.5~0.5 mrad；有螺线管存在的情况下，工作点落在和共振线时，将导致束流不稳定而大量损失，落在差共振线时，束流稳定。通过模拟计算发现：螺线管产生的耦合远大于磁铁的纵向角安装偏差产生的耦合。     

CSRm束流径向和轴向振荡的耦合

介绍了由于磁铁的安装误差和螺线管的存在而造成的束流径向和轴向的耦合，以及耦合对束流稳定的影响。结合CSRm结构的典型参数分析得出:二极磁铁和四极磁铁在纵向角安装偏差为-0.5~0.5 mrad；有螺线管存在的情况下，工作点落在和共振线时，将导致束流不稳定而大量损失，落在差共振线时，束流稳定。通过模拟计算发现:螺线管产生的耦合远大于磁铁的纵向角安装偏差产生的耦合。     

ADS强流质子加速器低能传输段发射度匹配研究北大核心CSCD

研制了一套强流质子源及低能传输线(LEBT)注入器用于ADS质子直线加速器。质子源产生35 ke V强流束经过低能传输段聚焦进入射频四极(RFQ)入口。低能传输段不匹配是强流RFQ中引起束流丢失的主要原因。不同加速段的束流匹配是减少束流损失与抑制发射度增长的重要手段。束流损失导致RFQ电极表面受热变形进而引起高频打火,降低RFQ长期运行的稳定性。针对以上问题,研究LEBT发射度在不同的实验条件下如何实现加速器更好的匹配。研究结果表明,LEBT出口束流在35 ke V,10 m A下,束流发射度小于0.2πmm·mrad,当LEBT螺线管电流为210和270 A时,束流在RFQ入口满足匹配条件。     

ADS强流质子加速器低能传输段发射度匹配研究

研制了一套强流质子源及低能传输线(LEBT)注入器用于ADS质子直线加速器。质子源产生35 ke V强流束经过低能传输段聚焦进入射频四极(RFQ)入口。低能传输段不匹配是强流RFQ中引起束流丢失的主要原因。不同加速段的束流匹配是减少束流损失与抑制发射度增长的重要手段。束流损失导致RFQ电极表面受热变形进而引起高频打火,降低RFQ长期运行的稳定性。针对以上问题,研究LEBT发射度在不同的实验条件下如何实现加速器更好的匹配。研究结果表明,LEBT出口束流在35 ke V,10 m A下,束流发射度小于0.2πmm·mrad,当LEBT螺线管电流为210和270 A时,束流在RFQ入口满足匹配条件。     

用于自由电子激光的S波段J型波导馈电加速管

随着波导式耦合行波加速管设计梯度的日益提高,为了防止加速管输入耦合器电场的横向动量在束流通过加速器耦合器时引起束流品质的下降,侧壁开有两个对称耦合孔的对称双馈圆柱腔获得了广泛的应用。研制的S波段J型波导馈电加速管即为双馈圆柱腔中的一种,研制样管在老练平台上老练时的最高加速梯度达到30 MV/m。然而因为四极场的存在,开有两个耦合孔的圆柱耦合腔内,仍然会引起轴向电场的幅度和相位在横向的梯度,从而使束流发射度变差。在理论上对J型波导馈电的跑道式耦合腔进行了研究,通过与圆柱腔进行比对模拟计算,证明跑道式耦合器可以很好地改善轴向电场在横向平面内非近轴区域沿圆周的场强一致性,从而减小四极场的影响。重要的是,J型波导馈电跑道式耦合腔的机械加工、测试比圆柱腔更加容易实现,是未来双馈加速器发展的一个理想方向。     

环形加速器中产生局部斜四极磁场的若干方法

本文研究了环形加速器中产生局部斜四极磁场的若干方法.它用来探索消除束流横向运动耦合所需要的斜四极磁场合适的方位和量值.并以BEPC为例,给出计算的结果.     

BEPCⅡ直线加速器发射度测量

BEPCⅡ直线加速器采用改变四极磁铁励磁电流, 测量获取的束流横截面荧光图像得到束流包络, 进而通过对束流包络和励磁电流的拟合计算得到束流发射度和Twiss参数. 在BEPCⅡ直线加速器的改进过程中, 发现并解决了影响发射度测量结果准确性的多个问题, 改进了束流横截面测量方法和发射度计算方法, 提高了测量结果的准确性. 根据BEPCⅡ直线加速器的具体情况, 还编写了束流截面测量程序和发射度计算程序, 提高了发射度的测量和计算速度, 方便了发射度测量实验的使用.     

BEPCⅡ直线加速器发射度测量

BEPCⅡ直线加速器采用改变四极磁铁励磁电流,测量获取的束流横截面荧光图像得到束流包络,进而通过对束流包络和励磁电流的拟合计算得到束流发射度和Twiss参数.在BEPCⅡ直线加速器的改进过程中,发现并解决了影响发射度测量结果准确性的多个问题,改进了束流横截面测量方法和发射度计算方法,提高了测量结果的准确性.根据BEPCⅡ直线加速器的具体情况,还编写了束流截面测量程序和发射度计算程序,提高了发射度的测量和计算速度,方便了发射度测量实验的使用.     

BEPCⅡ的耦合补偿方案

根据工程设计的特点和难点，BEPCII储存环的耦合补偿采用了创新的设计思路. 探测器的螺线管磁场将得到对撞点两侧6块反螺线管的完全补偿，弧区内的斜四极磁铁将对全局耦合参数进行补偿与调节. BEPCII耦合补偿与耦合调节的方案以及方案的可行性评估将在本文中详细介绍.     

高压直流连续波光阴极注入器中发射度补偿

空间电荷效应是引起发射度增长的主要因素,特别是在高压直流连续波光阴极注入器中。分析了高压直流连续波光阴极注入器中线性空间电荷力的特点及其对电子束横向发射度的影响,并从理论上解析地研究了螺线管发射度补偿的原理及特点。最后利用Parmela程序对中国工程物理研究院高压直流连续波光阴极注入器的发射度补偿作了模拟计算。结果表明,束团电荷量为80 pC的电子束在350 keV高压直流电子枪出口处的横向归一化发射度为5.14 mmmrad,经过螺线管补偿后,其最小横向发射度变为1.27 mmmrad。电子束的发射度得到了很好的补偿。     

SOME METHODS OF PRODUCING LOCAL SKEW QUADRUPOLE FIELD IN ACCELERATOR RING

In this paper,some methods of producing local skew quadrupole field in accelerator ring are studied.It can be used to find the suitable positions and strength of skew quadrupole field to remove the coupling between horizontal and vertical oscillations of beam,Taking BEPC as an example,some calculated results are given.     

Simulation and analysis of the transverse spectrum in HIRFL-CSR

Particles in a storage ring oscillate in the longitudinal and transverse dimensions.Therefore,the signal that beam has generated can be analyzed in the frequency domain to extract many beam parameters,such as tune,momentum spread,emittance and their evolution with time and so on.In this paper,the transverse spectrum in HIRFI-CSR was simulated and analyzed under different conditions,including electron cooling,hollow electron beam,solenoid effect,the tune shift caused by power supply ripple and the misalignment between ion and electron beams.The result of the simulation shows that the longitudinal magnetic field of the electron cooling device should be compensated by a "compensation solenoid",and the power supply ripple must be controlled,otherwise the accumulation would be affected and the beam would be lost.     

Beam Dynamics Design of a 50 mA D~+ RFQ

A new 973 project was proposed by Peking University and Institute of Modern Physics of Chinese Academy of Sciences recently.The project requires a 50 mA,162.5 MHz,cw mode radio frequency quadrupole(RFQ)to accelerate the D~+ to 1 MeV.In a high-current linear accelerator,the strong space charge effect causes the growth of envelope and emittance along with heavy beam losses.In the beam dynamics design of this RFQ,beam envelope mismatching is discussed and a matching dynamics method is proposed to minimize the envelope and emittance growth.The influence of limiting current on the beam transmission is discussed and used in the optimization of transverse and longitudinal parameters.After the optimization,the beam transmission efficiency reaches higher than 98%.     

Coupling measurement and correction at the SSRF storage ring

Brightness is an important parameter for 3^rd generation light source. Correcting the emittance coupling is a realistic way to increase brightness without any additional equipment in a machine under operation. The main sources of emittance coupling are betatron coupling and vertical dispersion. At the SSRF storage ring, tune split and LOCO are used to measure the respective betatron and emittance coupling. Both of these sources can be corrected by skew quadrupoles. By measuring the skew quadrupole-coupling response matrix, betatron coupling can be changed from 0.014% to 2%. But the vertical dispersion changes at the same time. LOCO can find the suitable setting to correct simultaneously the betatron coupling and vertical dispersion. The emittance coupling can be reduced to 0.17% by this method. More simulations show the potential for smaller emittance coupling if more skew quadrupoles are employed.     

A particle-in-cell mode beam dynamics simulation of medium energy beam transport for the SSC-Linac

A new linear accelerator system, called the SSC-Linac injector, is being designed at HIRFL (the heavy ion research facility of Lanzhou). As part of the SSC-Linac, the medium energy beam transport (MEBT) consists of seven magnetic quadrupoles, a re-buncher and a diagnose box. The total length of this segment is about 1.75 m. The beam dynamics simulation in MEBT has been studied using the TRACK 3D particle-in-cell code, and the simulation result shows that the beam accelerated from the radio frequency quadrupole (RFQ) matches well with the acceptance of the following drift tube linac (DTL) in both the transverse and longitudinal phase spaces, and that most of the particles can be captured by the final sector focusing cyclotron for further acceleration. The longitudinal emittance of the RFQ and the longitudinal acceptance of the DTL was calculated in detail, and a multi-particle beam dynamics simulation from the ion source to the end of the DTL was done to verify the original design.     

光阴极微波电子枪中发射度补偿及模拟计算

介绍了上海深紫外自由电子激光用光阴极微波电子枪采用发射度补偿技术的结果 .详细分析了线性空间电荷力的特点及对束流发射度的影响 ,从束流动力学和相空间两方面讨论了发射度补偿原理 .给出了补偿线圈的设计结构及其轴向场分布 .利用PARMELA程序对补偿效果作了模拟计算 .结果表明 ,设计的腔体对单圈 1 .5nC束团 ,在枪出口后 1 .2m处 ,电子能量为 5 .7MeV ,横向归一化发射度εn ,RMS=1 .61 2πmm·mrad. The emittance compensation technology will be used on the photo cathode RF gun for Shanghai SDUV FEL. In this paper, the space charge force and its effect on electron beam transverse emittance in RF gunis is studied, the principle of emittance compensation in phase space is discussed. We have designed a compensation solenoid and calulated its magnetic field distribution. Its performance has been studied by the code PARMELA. A simulation result indicates that the normalized transverse RMS emi...     

Simulation and analysis of the transverse spectrum in HIRFL-CSR

Particles in a storage ring oscillate in the longitudinal and transverse dimensions. Therefore, the signal that beam has generated can be analyzed in the frequency domain to extract many beam parameters, such as tune, momentum spread, emittance and their evolution with time and so on. In this paper, the transverse spectrum in HIRFL-CSR was simulated and analyzed under different conditions, including electron cooling, hollow electron beam, solenoid effect, the tune shift caused by power supply ripple and the misalignment between ion and electron beams. The result of the simulation shows that the longitudinal magnetic field of the electron cooling device should be compensated by a “compensation solenoid”, and the power supply ripple must be controlled, otherwise the accumulation would be affected and the beam would be lost.     

基于螺线管扫描法进行电磁叠加场中热发射度测量的仿真分析

在一种猝发高重频的X射线自由电子激光（XFEL）装置中,由于受到光阴极注入器内补偿螺线管与电子枪之间特殊结构的限制,阴极附近电场与磁场为叠加状态。实验中需要对阴极热发射度进行测量,而测量热发射度常用的螺线管扫描法基于几何发射度不变的前提,无法直接应用于电磁场叠加的结构。针对这一问题,考虑到归一化过程可以剔除电场对发射度的影响,基于此,研究归一化相空间中应用的螺线管扫描法,并通过仿真计算与分析,最终证明该方法适用于电磁叠加场中阴极热发射度的测量。