损失阻抗测量装置数据采集处理系统研制

电子储存环中真空部件的损失阻抗是表征该元件性能的重要参数,该参数的测量对于真空部件的设计,性能评估都有很大的意义。介绍了合肥储存环二期工程中损失阻抗测量的研制情况。     

7kA闸流管脉冲调制器的可编程控制器控制

利用ＰＬＣ（可编程控制器）作为冲击磁铁脉冲调制器的设备控制器,解决了大电流脉冲放电对设备控制器的干扰问题,实现了调制器的计算机遥控操作及联锁保护功能、实时通讯功能,提高了调制器实验装置运行的可靠性。     

冲击磁铁误差对注入过程的影响

简要说明合肥同步辐射光源（ＨＬＳ）的储存环新注入系统,分析由于冲击磁铁的误差而产生的非理想凸轨以及对注入过程的影响。针对ＨＬＳ的三种运行模式进行计算机模拟,从而确定冲击磁铁的误差极限。     

快速冲击磁铁系统的研制

合肥同步辐射光源（Hcfci Synchrotron light sourcc,HLS)的某些实验需要长时间间隔同步辐射（Synchrotronradiation)光脉冲，但是目前HLS还不能满足这些要求。因此提出在HLS储存环上采用局部凸轨的方法来延长SR光脉冲的时间间隔。为此设计了快速冲击磁铁系统，其中脉冲调制器采用脉冲成型线(Pulse Forming Line）技术设计；冲击磁铁为空芯电流板结构的磁铁。初步实验表明，快速冲击磁铁系统的设计符合实验要求。     

电子储存环扭摆磁铁效应的一种补偿方法

本文介绍BEPC储存环插入一块高场水平扭摆磁铁情况下一种可能的补偿方法。利用位于扭摆磁铁附近消失差区域中的由独立电源供电的四块四极磁铁,按Twiss参量重新匹配的要求改变其强度,在扭摆磁铁和四块四极磁铁所在区域及其以外区域,均可获得Twiss参量补偿的满意结果。     

HLS脉冲八极磁铁注入方案设计与研究

脉冲多极磁铁注入方法是近年来储存环上新兴的一种束流注入方案,具有注入元件少和对储存束流扰动小等优点。本文研究了在合肥光源(Hefei Light Source,HLS)上储存环采用单块脉冲八极磁铁实现束流注入的设计方案。通过物理过程推导和计算,在储存环上选择合适的八极磁铁的安装位置,初步确定相应的磁铁参数。对注入过程进行跟踪模拟,结果验证了注入束流的存活效率较高,对于储存束流的扰动比脉冲四极磁铁和脉冲六极磁铁注入方法更小,证明了在HLS上采用单块脉冲八极磁铁完成注入过程是可行的。     

合肥先进光源注入非线性冲击磁铁设计研究

合肥先进光源(Hefei Advanced Light Facility,HALF)是第四代衍射极限储存环型光源,其同步辐射光在真空紫外与软X射线波段.合肥先进光源的预研项目正在进行中,目前的注入系统拟采用非线性冲击磁铁的离轴注入方案,并处于重点考虑中.针对合肥先进光源项目,设计并研制了一种新型的适用于低发射度储存环的...     

HLS脉冲四极磁铁注入方法设计与研究

介绍了一种采用脉冲四极磁铁实现储存环束流注入的新方法.通过物理计算和注入过程数值模拟研究,确定了储存环上安装脉冲四极磁铁的位置和强度,并通过模拟计算评估了注入过程中注入束流存活效率和对储存束流的影响,证明了在合肥光源采用脉冲四极磁铁完成束流注入过程的可行性.     

CSNS/RCS陶瓷真空盒热特性及振动研究

陶瓷真空盒作为中国散裂中子源（CSNS）快循环同步加速器（RCS）真空系统的关键部件,能避免RCS二极、四极交流磁铁因快速变化的磁场而产生的涡旋电流。因安装空间限制,RCS陶瓷真空盒支架固定在磁铁线圈上。在CSNS/RCS交流磁铁长时间加电测试中,出现陶瓷真空盒断裂、真空破坏的情况。为避免后期出现类似问题,从磁铁发热进而引起陶瓷真空盒不均匀升温的角度出发,对陶瓷真空盒的热特性进行了分析,同时基于双目视觉测量技术,对陶瓷真空盒的振动情况进行了监测,针对部分真空盒水平方向振动异常的问题,确定其影响因素为快卸链条的磁导率超标。最后开展了陶瓷真空盒的支架减振技术研究。     

CSNS四极陶瓷真空盒磁控溅射镀TiN膜研究

介绍了中国散裂中子源（CSNS）快循环同步加速器（RCS）中四极陶瓷真空盒内表面镀TiN膜技术与成膜系统装置。采用磁控溅射法,通过在绝缘体长直管道外表面安装金属屏幕罩来提供同轴电场的方法,解决了镀膜均匀性的问题。镀膜样品Ti、N比在0.9~1.1范围内,膜厚为100nm左右,附着力达到要求,总体满足设计指标,完成了CSNS四极陶瓷真空盒样机的镀膜。     

阻抗匹配靶制备及靶参数精密测量

通过精密轧机轧制Al、Cu、Au等高纯金属箔片,采用精密微装配技术获得应用于激光状态方程实验所需的阻抗匹配靶。运用台阶仪和白光干涉仪分别对阻抗匹配靶进行靶参数精密测量。在“神光Ⅱ”上进行阻抗匹配的实验打靶,获得了相关靶型的实验图像。     

医用重离子加速器薄壁真空室研制

中国科学院近代物理研究所研制的医用重离子加速器装置是我国第1台拥有自主知识产权的医用重离子加速器,其高频脉冲二极磁铁使用RAMPING工作模式且磁场上升速率为1.6 T/s,所以安装在高频脉冲磁铁内的真空室采用一种薄壁加筋结构不锈钢真空室以减少涡流对离子束稳定性的影响。然而由于薄壁加筋不锈钢真空室占用磁铁气隙尺寸偏大,不仅造成了磁铁造价成本偏高,更是提高了运维成本。基于以上原因,本文提出陶瓷内衬薄壁（0.3 mm）真空室,并研制了原理样机。测试结果表明：样机真空度进入了10^-10 Pa量级范围,并可有效减小磁铁气隙,是未来加速器薄壁真空室的发展方向。     

Development of Thin-wall Vacuum Chamber for Heavy Ion Medical Accelerator

Heavy Ion Medical Machine (HIMM), developed by the Institute of Modern Physics, Chinese Academy of Sciences, is the first medical heavy ion accelerator with independent intellectual property rights in China. Because the RAMPING mode was used for high frequency pulse dipole magnets of HIMM and the rising rate of magnetic field is 1.6 T/s, the vacuum chamber installed in the high frequency pulsed magnet is a thin-wall stainless vacuum chamber with reinforcing ribs to reduce the influence of eddy current on the ion beam stability. However, the gap size of magnet occupied by thin-wall stainless vacuum chamber with reinforcing ribs is too large, and it not only causes the high cost of magnets, but also greatly improves the maintenance cost. Based on these reasons, a new thin-wall vacuum chamber (0.3 mm) with ceramic lining was put forward and the prototype was designed and manufactured. The test results show that the obtained pressure of the prototype is in the order magnitude of 10^-10 Pa, and the magnet gap can be effectively reduced. And it is the development direction of thin-wall vacuum chamber of accelerator in the future.     

Estimation of Electron-loss and Photon-scattering Corrections for Parallel-plate Free-air Chambers

Parallel-plate free-air ionization chambers are used for X-ray air-kerma rate standards at the National Metrology Institute of Japan (NMIJ), AIST. The electron-loss and photon-scattering correction factors are needed for the evaluation of air-kerma rate from measured current. The electron-loss correction factor (K_e) is a correction of the charge loss by giving energy to the electrode part without the high-speed electron stopping in the air area where the charges are collected. The scattering correction factor (K_sc) is for a correction of extra charges produced by scattered photons generated after an incidence photon is interactive. The electron-loss and photon-scattering correction factors for 3 different size parallel-plate free-air chambers are estimated by the EGS4 code. One chamber is used to get primary standards for absolute measurements of air kerma in beams of medium-energy X-rays and the other two are used for the same purpose in beams of low-energy X-rays. These correction factors are calculated for mono-energetic photons. It is found that electron-loss and photon-scattering correction factors depend on the chamber size, and the latter especially changes greatly depending on the size. The K_e and K_sc value for medium-and low-energy X-ray fields at AIST are estimated by averaging the energy deposition contributions over the X-ray spectrum.     

球形石墨空腔电离室壁修正因子的Monte-Carlo模拟和实验测量

采用Monte-Carlo模拟和实验测量两种方法对30cm³球形石墨空腔电离室在⁶⁰Coγ射线下的壁修因子Kwall进行研究。实验和模拟计算结果的比较表明，传统的线性外推法确定的壁修正能基准组的30cm³和50cm³球形石墨空腔电离室在⁶⁰Coγ射线下的相对电离电流和壁修正因子进行了Monte-Carlo模拟计算，计算的相对电离电流值与NIST发布的实验测量值在0.12%内吻合。     

岩性密度测井仪的研制

此测井仪包括井下探测仪器及地面计算机数据获取与控制管理系统。此仪器的测量范围:光电因子最大为33巴/电子,体密度1.9—2.9g/cm~3。测量精度:光电因子的相对误差小于±6％,密度的绝对测量偏差<±0.03g/cm~3。井下仪器能在井深3500m下正常工作。     

HP(10)次级标准电离室几个重要性能测量及模拟计算

介绍了T34035型H_p(10)次级标准电离室的结构和技术特性,实验测量了H_p(10)次级标准电离室的校准系数N_H和修正因子k(R,α),并评定给出校准系数N_H的相对扩展不确定度为4.6%(k=2),修正因子k(R,α)的相对扩展不确定度为6.0%(k=2)。在辐射质入射角≤75 °时,12～1 250 keV范围内能量响应好于±20%;个人剂量当量率非线性在100 μSv/h～3 Sv/h范围内好于±3%。采用 MCNP5模拟计算了该电离室对部分窄谱N系列和低空气比释动能L系列的k(R,α)值,结果表明计算值与实验测量值之间的相对误差在±6%范围内。说明该电离室性能满足次级标准电离室要求,可以直接用于H_p(10)量值的传递。     

Development of Thin Film Thermometer and Its Application to Radiation Loss Measurement in JFT-2 Tokamak

A thin film thermometer with high sensitivity and small response time has been developed. A nickel film was deposited in a vacuum on a backing plate of stainless steel 0.05 mm thick. The pattern of nickel film was so designed to provide sufficient accuracy. A small heat flux of 0.5 W/cm² is measurable with a response time of less than 1 ms. The thermometer was applied to radiation loss measurement in JFT-2 tokamak. The power loss due to the radiation was found to be about 30% of the total power input.