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针对北京正负电子对撞机改造工程(BEPC II)直线加速器束流位置测量电子学系统故障率上升这一现状,结合BEPC II直线加速器束流参数以及BPM电子学ADC芯片带通采样的需求,设计了隔离度高、幅相一致性好的数字BPM射频前端电子学模块。数字BPM电子学系统采用MicroTCA 4.0系统架构,以FPGA作为主控制器,基于EDA软件开发设计。重点介绍了射频前端电子学模块中射频功率放大器、数字可调衰减器、带通滤波器等设计和实验室及在线测试结果。BEPC II对撞模式下,使用正电子束流,完成电子学系统在线测试,x方向位置测量精度约为38.46 μm,y方向位置测量精度约为26.16 μm,其测量精度和系统稳定性优于商用模拟BPM电子学模块,能够满足BEPC II直线加速器束流位置测量需求。 相似文献
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为了高效地对直线加速器输出束流能量进行调节,设计了合肥光源(HLS-II)直线加速器束流能量调节方案。该方案在调试阶段通过能谱分析系统观察束团状态并测量束流能量,储存环注入阶段使用3个束流位置探测器(BPM)对束流能量进行在线测量;使用自动相位扫描程序对速调管输出相位进行扫描,获得各加速段的能量增益公式;定量调节速调管的输出相位和高压,实现直线加速器输出束流能量的快速调节。在线应用结果表明,该方案能快速实现束流能量调节,调节后的束流具有良好品质,束流横向能散小于0.22%,注入速率明显改善。 相似文献
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在合肥光源(HLS)升级改造中,为了增强注入器的束流位置检测器(BPM)系统的整体性能,采用单次通过数字束流位置处理器(Libera Brilliance Single Pass)构成信号处理系统。首先对Libera Brilliance Single Pass进行了离线的性能测试,然后用它对条带BPM进行实验台标定,最后在合肥光源现有200 MeV直线加速器上进行了在线测试。结果显示其离线分辨力为4~17 m,优于原有对数比处理系统。在线水平和垂直分辨力分别好于26 m和19 m,优于原有系统的58 m和33 m。 相似文献
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上海软X射线自由电子激光装置(SXFEL)对束流发射度增长的幅度有着较为严格的限制,传统的光学准直已经不能满足其要求。采用基于束流的准直方法可以实现更为精密的准直,使得直线加速器的准直误差进一步降低,以满足自由电子激光装置的要求。通过对不同条件下束流位置检测器(BPM)测得的数据采用最小二乘法算法进行计算分析,可以计算得到四极磁铁和BPM的准直误差,进而进行束流准直和轨道校正。基于以上原理,计算了各种元件误差对轨道和发射度造成的影响,同时基于Matlab平台设计了控制软件,模拟结果表明轨道偏离量可减少一个数量级。 相似文献
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合肥光源直线加速器BPM系统的研制和测量 总被引:1,自引:0,他引:1
合肥光源直线加速器新改造的BPM系统已经安装, 并做了在线的束流位置测量实验. 本文介绍该BPM系统的结构、作为系统核心部分的信号处理模块以及离线标定的实验结果和在线应用的实验结果, 表明该BPM系统具有不小于40dBm的动态范围, 不大于100μm的束流位置分辨率, 水平方向和垂直方向分别具有1.61dB/mm和1.51dB/mm的灵敏度. 校正铁强度与BPM读数关系的实验, 表明该BPM系统能正确地反映束流的位置变化情况, 并且确定了校正铁在水平方向和垂直方向的校正系数分别为0.46mm/A和0.58mm/A, 校正铁设置为默认值时该BPM处的束流中心水平位置和垂直位置分别为0.83mm和-0.57mm. 相似文献
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束流位置监测器(BPM)是粒子加速器束测系统中最为常见的元件,该探头输出信号中除包含束流位置信息外还包含电荷量等其它信息,可作为多参数束流诊断设备。采用BPM理论分析和数值仿真分析相结合的方法讨论了该种探头同时用于束流流强测量的可行性。在上海光源储存环上进行了束流试验,测定了全环140个BPM的流强标定系数,对BPM用于流强测量的分辨率、束流位置依赖性、频率依赖特性进行了测试,根据实验结果讨论了该方法在当前技术条件下所能达到的性能及其局限性。 相似文献
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在多脉冲强流直线感应加速器(LIA)的测控和诊断系统中,电子束的在线测试数据处理是重要的组成部分。多脉冲强流电子束在线测试数据处理系统是集测试仪器、计算机和工作站等组成的工业以太网,以及实现测试网络配置、测试仪器的通信及控制、数据采集、束流强度和束质心位置计算、显示以及存储等功能为一体的专用软件。多脉冲强流电子束采用基于电阻环束流位置检测器(BPM)的束流测试线路,根据束线上每个BPM测试得到的四个象限点的原始电压信号波形,以及测试线路的结构参数,计算束线上每个PBM位置的束流强度以及束质心位置随时间变化的波形,根据随时间变化的波形数据计算每个BPM位置多个脉冲束流的强度以及束质心位置的统计数据。数据的存储采用SQL和文件系统相结合的方式。这套多脉冲强流电子束在线数据处理系统在多脉冲强流LIA的调试实验中稳定可靠运行,为实验提供有效可靠的数据。 相似文献
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束流轨道对加速器的运行很重要,为了能准确的测量束流的位置,有必要对束流位置监视器(BPM)本身进行快速,准确的准直.介绍在BEPC上用束流作为基准来测量BPM的零点偏差(OFFSET) .这套测量系统用辅助绕组来改变四极磁铁的强度,已经应用到BEPC上,并且取得一定效果. 相似文献
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In this paper, the 2-D electrostatic field software, POISSON, is used to calculate the characteristic impedance of a BPM (beam position monitor) for a high current proton linac. Furthermore, the time-domain 3-D module of MAFIA with a beam microbunch at a varying offset from the axis is used to compute the induced voltage on the electrodes as a function of time. Finally, the effect of low 13 beams on the induced voltage, the sensitivity and the signal dynamic range of the BPM are discussed. 相似文献
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The RIA facility driver LINAC consists of about 400 superconducting (SC) independently phased rf cavities. The LINAC is designed
to accelerate simultaneously several charge-state beams to generate as much as 400 kW of uranium beam power. The LINAC beam
dynamics is most sensitive to the focusing and accelerating structure parameters of the pre-stripper section, where the uranium
beam is accelerated from 0.17 keV/u to 9.4 MeV/u. This section is designed to accept and accelerate two charge states (28
and 29) of uranium beam from an ECR ion source. The pre-stripper section must be designed to minimize the beam emittance distortion
of this two-charge-state beam. In particular, the inter-cryostat spaces must be minimized and beam parameters near transitions
of the accelerating and focusing lattices must be matched carefully. Several sources of possible effective emittance growth
are considered in the design of the pre-stripper section and a tolerance budget is established. Numerical beam dynamics studies
include realistic electric and magnetic three-dimensional field distributions in the SC rf cavities and SC solenoids. Error
effects in the longitudinal beam parameters are studied. 相似文献
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The optical projection using speckles is one of the structured light methods that have been applied to three-dimensional (3-D) range sensors. This paper investigates the design and fabrication of diffractive optical elements (DOEs) for generating the light field with uniformly distributed speckles. Based on the principles of computer generated holograms, the iterative Fourier transform algorithm was adopted for the DOE design. It was used to calculate the phase map for diffracting the incident laser beam into a goal pattern with distributed speckles. Four patterns were designed in the study. Their phase maps were first examined by a spatial light modulator and then fabricated on glass substrates by microfabrication processes. Finally, the diffraction characteristics of the fabricated devices were verified. The experimental results show that the proposed methods are applicable to the DOE design of 3-D range sensors. Furthermore, any expected diffraction area and speckle density could be possibly achieved according to the relations presented in the paper. 相似文献
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It is proposed to construct a spallation neutron source (SNS) at Centre for Advanced Technology (CAT) based on a 1 GeV proton
synchrotron with 100 MeV H− LINAC as injector. Additionally, the LINAC can form the first 100 MeV part of a 1 GeV proton LINAC to be built in future
for accelerator driven system (ADS) applications. We are exploring a configuration of the 100 MeV LINAC which will consist
of an H− ion source, a 4–6 MeV RFQ followed either by a 20 MeV drift tube LINAC (DTL) and 100 MeV separated function drift tube LINAC
(SDTL) or a coupled cavity drift tube LINAC (CCDTL) structure. In this paper, we present the results of our preliminary physics
design studies of the RFQ-SDTL, RFQ-CCDTL and RFQ-DTL-SDTL configurations. The design of the 4.5 MeV RFQ is discussed along
with the matching sections between the RFQ-SDTL/DTL and RFQ-CCDTL. The choice of the accelerator configuration and that of
various parameters of the individual accelerator structures under consideration are discussed. The design objectives are to
arrive at a configuration which eases heat removal for CW operation and which is less prone to halo formation in order to
reduce the beam loss at higher energies. 相似文献
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The Electron LINAC Department 《中国物理C(英文版)》1988,12(3):365-371
The beam test of the 250MeV section of BEPC 1.1/1.4GeV e± LINAC was performed four times during its installation phase.In May of 1987,electron beam of 760mA and 250MeV was obtained and positron beam current of 2.5mA and 99MeV was observed when an electron beam of 785MeV bombarding a tungsten target.The main parameters of LINAC met the design values and achieved the same technical level of similar accelerators in other countries. 相似文献
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P N Ostroumov 《Pramana》2002,59(6):895-913
The Nuclear Science Community in the Unites States has unanimously concluded that developments in both nuclear science and
its supporting technologies make building a world-leading Rare-Isotope Accelerator (RIA) facility for production of radioactive
beams the top priority. The RIA development effort involves several US Laboratories (ANL, JLAB, LBNL, MSU, ORNL). The RIA
facility includes a CW 1.4 GeV driver LINAC and a 100 MV post-accelerator both based on superconducting (SC) cavities operating
at frequencies from 48 MHz to 805 MHz. An initial acceleration in both LINACs is provided by room temperature RFQs. The driver
LINAC is designed for acceleration of any ion species; from protons up to 900 MeV to uranium up to 400 MeV/u. The novel feature
of the driver LINAC is an acceleration of multiple charge-state heavy-ion beams in order to achieve 400 kW beam power. Basic
design concepts of the driver LINAC are given. Several new conceptual solutions in beam dynamics, room temperature and SC
accelerating structures for heavy ion accelerator applications are discussed. 相似文献
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S Ghosh R Mehta P N Prakash A Mandal G K Chaudhari S S K Sonti D S Mathuria K K Mistry A Rai S Rao P Barua A Pandey B K Sahu A Sarkar G Joshi S K Datta R K Bhowmik A Roy 《Pramana》2002,59(5):881-884
An on-line test of the LINAC superbuncher at Nuclear Science Centre has been successfully performed. DC O7+ beam of nominal energy 92 MeV was accelerated through the superbuncher resonator, operating at a field of 4.54 MV/m. The
total energy gain of the beam was measured to be 4.5 MeV. For the pulsed beam test a phase locked bunched beam of O7+ of nominal energy 92 MeV, FWHM 1.3 ns from the pre-tandem multiharmonic buncher was injected into the superbuncher. By properly
adjusting the phase and amplitude of the resonator, the best FWHM of the bunched beam was measured to be 185 ps near the entrance
of the first LINAC module. Fully depleted cooled surface barrier detector was used for measuring the time width. In a separate
experiment the intrinsic time resolution of the same detector was measured to be 134 ps. Consequently the intrinsic time width
of the bunched beam, after correcting for the detector resolution, would be 127 ps. Details of the experiment and results
are presented. 相似文献