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HIRFL-CSR Tune值测量系统 总被引:2,自引:1,他引:1
兰州重离子加速器冷却储存环(HIRFL-CSR)工作点(Tune)测量系统已投入调束运行.采用FFT测量法,用白噪声信号做激励源,经功率放大并通过同轴开关切换将激励信号加载到垂直或水平的对称极板上,通过位置检测器(BPM)采集束流信号.将BPM两极板感应到的束流信号分别经前置放大器放大,再通过相位相差180°的合路器将差信号送入实时频谱仪进行傅里叶分析,从而计算出Tune值.本文主要介绍HIRFL-CSR工作点测量原理、系统构成以及测量结果. 相似文献
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设计了一套用于测量超导增能器束流能量的系统,并专门加工了测量装置,束流经准直后轰击金靶,通过测量散射粒子确定束流能量.探测器采用金硅面垒型半导体探测器,其信号经放大处理后进入多道分析器测量散射粒子能谱.另外基于Lab VIEW开发平台,编写了测控软件,完成了束流能量刻度、能量测量和工作相位设置,并采用CA Lab方式与... 相似文献
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针对加速器驱动次临界系统(Accelerator Driven Sub-critical System,ADS)注入器Ⅰ束流调试要求,需要精确测量束流的相位和能量。本文研究束流的相位和能量高精度测量方法,设计了基于快速电流变压器(Fast Current Transformer,FCT)信号的相位及能量测量系统。该系统包括FCT探头、前端电子学、数据采集和处理三个部分,通过正交采样的方式实现束流的相位测量,然后利用飞行时间法实现束流能量的测量。测试结果表明,该系统在实验室测试相位分辨率为±0.8°,在线测试相位分辨率为±2°,满足直线加速器的设计要求。 相似文献
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上海软X射线自由电子激光装置(Shanghai Soft X-ray Free Electron Laser, SXFEL)需1个分辨率达到亚μm量级的束流位置测量系统,并采用基于束流准直的方法实现波荡器段电子束与光子束的紧密重合。为此设计研制了1个由C波段腔式探头、单路混频至低中频的射频前端以及自主研发的专用数字信号束流位置处理器(digital beam position monitor processor, DBPM)构成的腔式束流位置测量(cavity beam position monitor, CBPM)系统。本文对系统的设计、软硬件结构、系统搭建进行了介绍,并基于漂移段搭建的3个紧邻的CBPM阵列完成了在线系统性能评估。束流实验结果表明,在束团电荷量为500 pC、系统动态范围在±800 μm的条件下,位置分辨率可达880 nm,这也是国内首次研制成功可在线运行的具有亚μm位置分辨率的CBPM系统。此外,采用CBPM的相位腔进行相对束团电荷量、束团到达时间的测量,其性能评估结果也均优于SXFEL设计要求。 相似文献
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介绍了中国散裂中子源(CSNS,China Spallation Neutron Source)质子加速器DTL(Drift Tube Linac)束流相位和能量测量系统的数据获取系统的设计。在该系统中,基于Nios Ⅱ嵌入式系统及100 M以太网口来实现命令和数据的传输,使得该系统成为一个独立的束流相位测量及数据传输仪器系统,极大地简化了系统的结构。 相似文献
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《核技术》2015,(10)
针对上海光源机器故障分析的需求,对原有储存环束流轨道联锁系统进行升级,实现对储存环束流位置测量系统中140台束流位置监测器(Beam Position Monitor,BPM)电子学输出的联锁信号进行标记,同时锁存丟束过程中所有BPM电子学中的逐圈轨道数据。联锁信号的处理与锁存触发信号的输出在FPGA(Field Programmable Gate Array)内完成。该系统集成至储存环的物理实验与工业控制系统(Experimental Physics and Industrial Control System,EPICS)控制系统之中。束流检测实验表明,该系统能够准确区分不同BPM电子学输出的联锁信号,同时锁存丟束时逐圈轨道数据,并通过该系统观测到了储存环束流丢失过程中的逐圈轨道变化。 相似文献
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W. Gebhardt 《Nuclear Engineering and Design》1983,76(3):275-283
Methods for defect reconstruction and classification using the flexible and fast electronic beam forming with phased arrays have been described. Using the electronic sector scan, a reflecting point is represented as a short circular curve, the length of which is dependent upon beam width and system sensitivity. By superimposing all sector displays on a storage tube, a defect is reconstructed by the inner envelope of the circular curves. If, instead of the circular curves, only their centers (intensity maxima) are recorded, a defect is reconstructed by individual image points. This representation has the important advantage that is to a large extent independent of beam width and system sensitivity. The reconstruction by compound scanning which includes, as a special case, the conventional focused probe technique with B-scan presentation, has a high redundancy; and in the case of testing coarse grained materials, the coherent noise is essentially reduced (intensity averaging). By recording the maximum echo height during sector scanning with open beam, a compound scan amplitude-locus curve (VAOK) is generated which represents the directivity of the defect. 相似文献
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In normal experimental operation, a diagnostic neutral beam (DNB) can produce 6 A of extracted beam current in hydrogen at an energy of 49 keV with a pulse length of 100 ms. Hydrogen and deuterium beams can be produced as well. The diagnostic neutral beam has been added to the diagnostic set so that charge-exchange recombination spectroscopy (CXRS) can be used to acquire ion temperature and rotation. The beam power and beam profile distribution of the DNB injection can be obtained with a thermocouple probe measurement system on the HT-7 superconducting tokamak. The thermocouple probe measurement system with 13 thermocouples crossly distributed on the probe plate was used to measure the temperature rise of each coppery target, so the profile distribution of the ion/neutral beam was obtained by calculation. In this paper, the structure of the probe plate on the DNB for HT-7 tokamak and some measurement results are presented. 相似文献
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利用一个三维环形探针对离子束进行旋转扫描,可以同时测量到两个束流截面的大小和位置,估算出二截面附近的聚焦梯度以及束腰的移动。 相似文献
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S. Lebed M. Tolmachov O. Kukharenko O. Veselov 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2009,267(12-13):2013-2016
The modified Van de Graaff accelerator with proton beam energy W ? 3 MeV has been installed and put into operation at the TMM laboratory in Kiev. The laboratory incorporates the nuclear probe (NP) beam line, coupled to this accelerator. A short version of an optimized probe-forming system (PFS) has been developed for the Kiev NP. The system is based on divided triplet of the magnetic quadrupole lenses (MQLs). This PFS has two working regimes for the probe operations. The results of numerical calculations of the geometrical and ion-optical parameters of the PFS are presented. It is shown that this versatile PFS is a promising design for a modern nuclear nano-probe. A new precision adjustable MQL has been designed. Three lenses, the slit systems and target chamber are manufactured and installed at the Kiev probe beam line. Also a new data acquisition system for the Kiev NP is being developed. 相似文献
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《IEEE transactions on nuclear science》2005,52(4):830-833
Real time monitoring of hadrontherapy beam intensity and profile is a critical issue for the optimization of dose delivery to carcinogenic tissue, patient safety and operation of the accelerator complex. For this purpose an innovative beam monitor, secondary electron emission for low interception monitoring (SLIM) is being developed in the framework of the EC-funded silicon ultra-fast cameras for electrons and gamma sources in medical application (SUCIMA) project. The detector system is based on the secondary emission of electrons by a nonperturbative, sub-micron thick Al foil placed directly in the extracted beam path. The secondary electrons, accelerated by an electrostatic focusing system, are detected by a monolithic silicon position-sensitive sensor, which provides the beam intensity and its position with a precision of 1 mm at a 10 kHz frame rate. The results of the laboratory tests of the first system prototype with thermoionic electrons emitted from a hot Tungsten wire are presented together with the measurements performed on a low intensity hadron beam at the Cyclotron of the Joint Research Centre in Ispra. 相似文献
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数字束流位置探测器(BPM)算法是数字BPM系统最核心的部分,其对束流位置测量的精度起决定作用。本文在完成数字BPM算法MATLAB模拟工作的基础上,将模拟优选出的数字BPM算法在自制的电子学硬件上进行FPGA实现。首先介绍了数字BPM算法的总体设计和实现方案;其次介绍了数字BPM算法各功能模块的设计原理及其在FPGA中的具体实现方法;最后在输入信号频率499.8 MHz、强度-10 dBm、BPM探头灵敏度系数23的条件下进行了实验室测试。实验结果显示:逐圈位置分辨达2.96 μm,快响应位置分辨达0.65 μm,闭轨位置分辨达0.33 μm,验证了本算法在束流位置测量中具有良好性能。 相似文献
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文章改变以往习惯于以离子束均方根半径等为控制变量的束晕-混沌模拟控制方法,取匹配半径外离子数与总离子数之比为控制变量,并构造一对数函数控制器,以进行束晕-混沌控制的模拟研究。结果显示,新的控制方法对强流加速器中5种初始分布的离子束均有较好的控制效果。由于此方法只需探测跨越匹配半径的离子数,在实验上有实施的可能。 相似文献
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