加速器驱动次临界系统注入器Ⅰ束测系统（英）

加速器驱动次临界系统注入器Ⅰ,包括ECR离子源、低能传输线、射频四极加速单元、中能传输段和超导腔,注入器Ⅰ出口能够获得能量10 MeV的强流质子束流。为了调束和运行的需要,注入器Ⅰ将安装束流位置测量、束流截面测量、束流流强测量、束流发射度和能量测量,以及束流损失测量等束流参数测量装置。介绍了这些束流测量系统设计及其他方面的一些考虑。     

任意形状束流相空间变换的样条函数表述

为了研究具有任意形状相空间的束流的传输,本文提出了束流相空间换的样条函数表述.利用三次样条函数拟合相空间边界,将相空间变换化为样条函数的变换,并进而计算束流包络.给出了具有任意形状相空间的束流传输的实例.     

“神龙一号”加速器束流输运系统研制

文章系统介绍了“神龙一号”直线感应加速器束流输运系统的研制过程和取得的成果, 重点阐述了螺线管线圈、二极校正线圈、多功能腔等关键单元部件的设计、传输元件的磁轴测量和准直安装、束线的总体布局、束流调试等研究内容. 束流调试结果表明, 该束流传输线的设计是成功的, 并且具有较宽的动态适应范围. 最后, 结合束流调试的经验, 提出了一些建议供以后工作参考.     

加速器束流诊断技术的新进展

介绍了加速器束流诊断技术的新进展, 包括束流位置测量技术、束团横向尺寸测量技术和束团长度测量技术. 束流位置测量技术主要介绍具有高位置分辨率的腔型束流位置检测器和数字束流位置处理技术. 束团尺寸测量技术主要介绍高空间分辨率的激光丝扫描器、光学渡越辐射和光学衍射辐射技术. 束团长度测量技术主要介绍高时间分辨率的相干辐射光谱技术、RF横向偏转腔、RF零相位技术和电光采样技术.     

HLSⅡ新的注入器束流强度测量系统

合肥光源升级改造任务已基本完成,注入器实现满能量注入。为适应新的注入器束流强度的测量需求,设计了新的注入器束流强度测量系统,该系统利用安装在真空腔上的3个快速束流变压器(FCT)和2个积分束流变压器(ICT),能够实现束流流强和电荷量的非拦截实时测量。为了准确获取束流参数,首先对束流变压器(CT)传输电缆进行了在线和离线标定;由于ICT输出信号信号幅度较小,噪声大,设计了低噪声前置放大器以改善信噪比;考虑低频谐波噪声和Kicker噪声的干扰,软件中通过适当的算法对噪声进行了处理;最后给出了部分在线实验结果。实验结果表明,束流传输效率约为27.4%,注入效率约为44.3%。     

基于对数比电路的HLS turn-by-turn系统

 较详细地介绍了合肥光源逐圈束流位置测量(turn-by-turn)系统设计思想和理论分析。该系统是为了判定二期工程升级后的注入系统的注入效率和Damping率,研究Beta振荡和轨迹瞬时变化以及其他束流动力学问题如工作点变化等的研究而研制。选择了新近受到广泛重视的对数比电路服务束流瞬时位置信号的处理。利用工作在204MHz的对数比电路完成被激励束的turn-by-turn位置测量和相空间检测。给出了该系统各部分性能和理论分析结果，介绍了快速多通道ADC在该系统的数据获取中的应用。     

微带传输线束流信号展宽处理设计

对束流信号进行展宽处理是储存环逐束团位置测量RF前端设计的重要工作之一。针对上海光源储存环束流信号的特点，对束流信号展宽进行分析，采用低通滤波器和包络检波联合的方法对信号进行展宽。考虑到实现过程需要对信号进行ps量级的延时，使用微带传输线对该方法进行了具体设计。对微带传输线等效为集总参数LC元件进行推导以进行低通滤波器设计，给出了阻抗匹配方案以实现宽带功率分配器与合成器。仿真和实测结果表明，所设计的电路能够对束流信号进行有效展宽处理。     

光阴极RF腔注入器束流发射度研究

 分析了光阴极RF腔注入器中的RF场效应和空间电荷效应，给出了电子在加速腔中束流发射度的解析表达式，它说明在加速过程中束流发射度是振荡变化的。利用SUPERFISH和GPT程序模拟计算了光阴极1+1/2腔注入器输出束流发射度与加速场强、注入相位、束团大小和形状、束团电荷的关系。适当选择这些条件，可以获得横向发射度小于2πmm·mrad 的输出束流。     

升级的合肥光源闭轨测量系统及其应用

 描述了合肥同步辐射光源二期工程中，电子储存环升级的闭轨测量系统及其在设备研制中的应用。介绍了性能稳定可靠的Bergoz束流位置监测电子学信号处理器。升级后的闭轨测量系统中处理电子学电路的束流位置分辨率可达1μm，系统误差小于10μm。整个测试系统的分辨率小于3μm。利用该高精度闭轨测量系统和基于束流准直系统完成了束流准直四极铁磁中心的测量，并和控制系统完成了储存环全环闭轨反馈校正试验。一个完整的束流位置监测系统已投入了在线运行，保障了为用户提供高稳定高品质的光源。     

ADS注入器II的5 MeV高能传输线的设计与搭建

ADS先导专项的注入器Ⅱ计划在将质子束通过一个Cryomodule加速到5 MeV后,进行10 mA连续束流的调试,以验证ADS低能段的强流超导直线加速器技术。为了将50 kW的束流功率沉积到束流垃圾站,需要搭建一条高能束流传输线,从超导段开始传输束流。采用两套三组合四极透镜控制束流包络及垃圾站的束流尺寸,利用诊断真空室进行水平和垂直发射度的测量。为避免束流产生的真空管道损伤,该传输线必须确保束流无损失地传输到垃圾站。A CW 10 mA,5 MeV beam commissioning of CADS Injector Ⅱ is planed recently to test the high power superconduction linac techniques.To transport 50 kW beam from linac to the beam dump,a high energy beam line (HEBT) line is designed and setup.Two Triplet are used to control the beam size along HEBT and at the beam dump.One diagnostics box is used for horizontal and vertical emittance measurement.To avoid damages to the vacuum pipe,beam should be transported to the beam dump without losses.The details of the HEBT design will be described in the paper.     

an Introduction to Mebt For JKJ and Its Upgrade Design

The medium-energy beam-transport line (MEBT) plays an important role in reducing the beam loss in the Japan Proton Accelerator Research Complex (J-PARC). A MEBT was designed and constructed,with good beam matching and lower beam loss. A brief introduction to the MEBT and its beam test results are given. To further reduce the beam loss during the transient time of the chopper,a medium-energy beamtransport line with an anti-chopper has been designed. It accomplishes three tasks: matching the beam from the RFQ to the acceptance of the DTL, chopping the beam to produce gaps for injection into the rapid cycling ring which follows the linac, and returning the partially deflected beam back to the acceptance of the DTL. An RF chopper and an anti-chopper have been adopted in the beam line, and the optimization of the design of the chopper cavity is discussed. Details of the beam dynamics analysis are given.     

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.     

医用质子加速器注入器7 MeV漂移管直线加速器的设计

 针对质子治癌直线加速器功耗少、长度短的要求,设计了一台工作频率为324 MHz的漂移管型质子直线加速器(DTL)。该DTL把粒子从2.5 MeV加速到7 MeV,功耗为265 kW, 总长1.9 m。横向聚焦采用FODO结构,漂移管内放置永磁铁。提出一种新的束流匹配方案,在射频四极场加速器(RFQ)与DTL之间不设束运线,而是以 DTL入口处的4个单元为匹配段,把RFQ出口处相椭圆匹配到DTL周期结构入口处的相椭圆。 用PARMILA程序对该DTL进行了动力学模拟,结果表明该方案的束流发射度增长很小。     

Variations in bonding of iron in porous ferrisilicates

The ISAC post accelerator comprises an RFQ, DTL and SC-linac. The high energy beam lines connect the linear accelerators as well as deliver the accelerated beams to two different experimental areas. The medium energy beam transport (MEBT) line connects the RFQ to the DTL. The high energy beam transport (HEBT) line connects the DTL to the ISAC-I experimental stations (DRAGON, TUDA-I, GPS). The DTL to superconducting beam (DSB) transport line connects the ISAC-I and ISAC-II linacs. The superconducting energy beam transport (SEBT) line connects the SC linac to the ISAC-II experimental station (TUDA-II, HERACLES, TIGRESS, EMMA and GPS). All these lines have the function of transporting and matching the beams to the downstream sections by manipulating the transverse and longitudinal phase space. They also contain diagnostic devices to measure the beam properties.     

Study of the design of CSNS MEBT

The design of CSNS MEBT has two objectives: (1) to match the beam both in the transversal direction and the longitudinal direction from RFQ into DTL; (2) to further chop the beam into the required time structure asked by RCS. It is very difficult and critical to control well the emittance growth and in the meantime to match and chop the beam. Firstly, the optical design is done and optimized, and the multi-particle simulations show that the maximum emittance growth is successfully controlled within 14%. Secondly, based on the different beam envelopes obtained by TRACE-3D and PARMELA, the least deflecting angle of the chopper is determined by TRACE-3D. At last, the field of steering magnet is determined through simulations.     

Design and construction of the MEBT1 for CADS injector scheme Ⅱ

A Medium Energy Beam Transport line 1(MEBT1) has been designed for Injector Scheme II of the China ADS project. To match the beam from RFQ to Superconducting(SC) Half Wave Resonator(HWR) sections with emittance preservation, the MEBT1 has been designed to be mechanically compact. Working at 162.5 MHz,the MEBT1 transports a 10 m A, 2.1 Me V proton beam using seven quadrupoles and two bunching cavities within2.7 meters. Three collimators are placed between every two adjacent quadrupoles to collimate the beam halo. Design and construction of the MEBT1 are presented in this paper.     

The design and construction of a pulsed beam generation system based on high intensity cyclotron

In order to perform the studies on a pulsed beam generation system based on a high intensity cyclotron, a test beam line with a pulsed beam generation for a 10 MeV compact cyclotron (CYCIAE-10) has been designed and constructed at China Institute of Atomic Energy (CIAE). A 70 MHz continuous H-beam can be pulsed to the pulse length of less than 10 ns with a repetition rate of 4.4 MHz. The sine waveform with a frequency of 2.2 MHz is adopted for the chopper and a mesh structure with single drift and dual gaps is used for the 70 MHz buncher. A helical resonator is designed and constructed based on simulations and experiments on the RF matching for the chopper. A helical inductance loop that is exceptionally large of its kind and equipped with water cooling for the resonator has been successfully wound and a 500 W solid RF amplifier has been manufactured. A special measuring device has been designed, which can be used to measure both the DC beam and the pulsed beam. The required pulsed beam was obtained after pulsed beam tuning.     

The design and construction of a pulsed beam generation system based on high intensity cyclotron

In order to perform the studies on a pulsed beam generation system based on a high intensity cyclotron, a test beam line with a pulsed beam generation for a 10 MeV compact cyclotron (CYCIAE-10) has been designed and constructed at China Institute of Atomic Energy (CIAE). A 70 MHz continuous H-beam can be pulsed to the pulse length of less than 10 ns with a repetition rate of 4.4 MHz. The sine waveform with a frequency of 2.2 MHz is adopted for the chopper and a mesh structure with single drift and dual gaps is used for the 70 MHz buncher. A helical resonator is designed and constructed based on simulations and experiments on the RF matching for the chopper. A helical inductance loop that is exceptionally large of its kind and equipped with water cooling for the resonator has been successfully wound and a 500 W solid RF amplifier has been manufactured. A special measuring device has been designed, which can be used to measure both the DC beam and the pulsed beam. The required pulsed beam was obtained after pulsed beam tuning.

     

Accelerator development in India for ADS programme

At BARC, development of a Low Energy High Intensity Proton Accelerator (LEHIPA), as front-end injector of the 1 GeV accelerator for the ADS programme, has been initiated. The major components of LEHIPA (20 MeV, 30 mA) are a 50 keV ECR ion source, a 3 MeV Radio Frequency Quadrupole (RFQ) and a 20 meV drift tube linac (DTL). The Low Energy Beam Transport (LEBT) and Medium Energy Beam Transport (MEBT) lines match the beam from the ion source to RFQ and from RFQ to DTL respectively. Design of these systems has been completed and fabrication of their prototypes has started. Physics studies of the 20–1000 MeV part of the Linac are also in progress. In this paper, the present status of this project is presented.      

Study of the design of CSNS MEBT

The design of CSNS MEBT has two objectives：（1） to match the beam both in the transversal direction and the longitudinal direction from RFQ into DTL;（2） to further chop the beam into the required time structure asked by RCS. It is very diffcult and critical to control well the emittance growth and in the meantime to match and chop the beam. Firstly,the optical design is done and optimized,and the multi-particle simulations show that the maximum emittance growth is successfully controlled within 14%. Secondly,based on the different beam envelopes obtained by TRACE-3D and PARMELA,the least deflecting angle of the chopper is determined by TRACE-3D. At last,the field of steering magnet is determined through simulations.