聚乙烯导热复合材料的电子束辐照改性

将低密度聚乙烯(LDPE)、氧化铝(Al₂O₃)和纳米二氧化硅(SiO₂)进行熔融共混,再通过电子束辐照对得到的材料进行改性,得到了同时具有高导热性能和力学性能的复合材料(PE-Al-Si)。 当纳米SiO₂的质量分数为1%,电子束辐照剂量为120 kGy时,与不含SiO₂的复合材料(PE-Al)相比,PE-Al-Si的导热系数达到了0.759 W/(m·K),提高了22%。 另外,PE-Al-Si的拉伸强度比PE-Al提高了17%。 证明SiO₂不仅可以改善复合材料的力学性能,同时还提高了辐照效率及复合材料的导热性能。     

Effect on Landau damping rates for a non-Maxwellian distribution function consisting of two electron populations

In many physical situations where a laser or electron beam passes through a dense plasma,hot low-density electron populations can be generated,resulting in a particle distribution function consisting of a dense cold population and a small hot population.Presence of such low-density electron distributions can alter the wave damping rate.A kinetic model is employed to study the Landau damping of Langmuir waves when a small hot electron population is present in the dense cold electron population with non-Maxwellian distribution functions.Departure of plasma from Maxwellian distributions significantly alters the damping rates as compared to the Maxwellian plasma.Strong damping is found for highly nonMaxwellian distributions as well as plasmas with a higher density and hot electron population.Existence of weak damping is also established when the distribution contains broadened flat tops at the low energies or tends to be Maxwellian.These results may be applied in both experimental and space physics regimes.     

Electron beam evaporation deposition of cadmium sulphide and cadmium telluride thin films： Solar cell applications7

Cadmium sulphide （CdS） and cadmium telluride （CdTe） thin films are deposited by electron beam evaporation. Atomic force microscopy （AFM） reveals that the root mean square （RMS） roughness values of the CdS films increase as substrate temperature increases. The optical band gap values of CdS films increase slightly with the increase in the substrate temperature, in a range of 2.42-2.48 eV. The result of Hall effect measurement suggests that the carrier concentration decreases as the substrate temperature increases, making the resistivity of the CdS films increase. CdTe films annealed at 300 ℃ show that their lowest transmittances are due to their largest packing densities. The electrical characteristics of CdS/CdTe thin film solar cells are investigated in dark conditions and under illumination. Typical rectifying and photovoltaic properties are obtained.     

973 RFQ 水冷调谐系统(英文)

由于束流的传输效率对射频四极场加速器(RFQ) 中射频场的分布极其敏感,所以在RFQ 的运行过程中不再采用传统的调谐器调谐RFQ。水冷调谐的方法基本上不影响RFQ 射频场的分布,所以适用于RFQ 的调谐。中国科学院高能物理研究所为C-ADS、CSNS 预研RFQ 项目开发建造了一套水冷调谐系统,使用RF 相位差作为控制量进行RFQ 水冷调谐,相位差的控制精度达到了1°运行结果显示该系统满足了RFQ 的调谐需求。介绍了该系统的水冷系统、调谐控制系统和一些运行经验。Since the beam transmission of a Radio Frequency Quadrupole(RFQ) Accelerator is very sensitive to the field profile, the ordinary frequency tuning method by the local movable tuner is no more adopted in an RFQ operation. The tuning method by controlling cooling water temperature is widely adopted to tune the RFQ due to the less affect on the RFQ field profile. A Resonance Control Cooling System (RCCS) is developed and commissioned for the 973 RFQ,which is a R&D project for C-ADS and CSNS RFQ at IHEP. This system adopts the RF phase difference as control variable to tune the RFQ. The control accuracy of the RF phase difference is about 1°. The running of the 973 RFQ shows that the RCCS works very well and fully satisfies the operation requirement of the RFQ. In this paper, the water skid, resonance control system of the RCCS and the operation experiences will be presented.     

应用于在束PET的光纤链路设计

医用重离子加速器(Heavy-Ion Medical Machine,HIMM)中安装在束正电子发射断层扫描装置(In-beam Positron Emission Tomography,In-beam PET)可实现治疗时对肿瘤靶区的照射剂量和位置分布的实时监测功能.在束PET工作时,事件经探测器阵列采集,由前端数据...     

中国散裂中子源/快循环质子同步加速器射频同步相位环路的数字化控制

 介绍了中国散裂中子源/快循环质子同步加速器射频同步相位环路的数字化控制系统设计方案,并利用ALTERA公司的现场可编程门阵列开发面板进行了系统开发,完成了控制回路的编程与仿真,进行了桌面实验和低功率实验,并对其进行了分析与讨论。实验结果表明：同步相位环路运行稳定,控制误差小于1°,满足物理设计要求。     

PET回旋加速器内部束流测量探头热分析

 基于时域有限差分法（FDTD）对PET回旋加速器内部束流测量探头的热传导过程进行了数值模拟。定义了运动和固定两种探头测量模式,在辐射散热的条件下,分别研究了3种探头材料（铜、钽、钨）在两种模式下的表面最高温度和尾部温度随功率加载时间的变化。研究表明：运动模式下,3种探头材料没有明显的优劣,探头速度选为10 mm/s较为合适;固定模式下,由于铜材料具有高黑度、高热导率的优点,是设计探头的最佳材料。     

强流电子束加速器运行过程电磁辐射的实验研究

 强流电子束加速器运行时,临近的计算机和示波器会发生黑屏,这是由于在该过程中产生了较强的电磁辐射干扰。采用实验研究的方法,对实验室研制的强流电子束加速器产生的电磁辐射进行了测量和分析。结果表明：强流电子束加速器产生的电磁辐射主要来源于初级气体开关触发、初级气体开关导通以及气体主开关自击穿导通3个过程。其中,初级气体开关导通时辐射的电磁波强度较大,其强度最大处在与开关相同高度的位置。此外,强流电子束加速器在运行过程中的电磁辐射为低频辐射,主频为21 MHz。     

具有双电子束结构的双波段相对论返波振荡器粒子模拟研究北大核心CSCD

研究了一种能够同时产生C波段和X波段微波、具有双电子束结构的相对论返波振荡器,采用嵌套式的高频结构将两个波段的束-波相互作用空间隔离开来,从而使两个波段的束-波相互过程互不影响。当二极管电压为650kV、内外环形电子束流分别为5.4,6.4kA、导引磁场为2.2T时,两个波段微波的频率分别为4.625,8.450GHz,模拟产生的微波功率分别为920,600MW,转换效率约为21.8%,17.1%。并采用粒子模拟法研究了导引磁场、二极管电压及两个束-波相互作用区关键结构参数对器件运行的影响,给出了双波段微波功率、频率随导引磁场、二极管电压等参数的变化曲线。     

大直径钪酸盐阴极发射特性

 为获得kA级热发射电子束,研制了直径为100 mm钪酸盐热阴极组件,并建立了适应大面积热阴极实验环境的2 MV 注入器试验平台。实验在二极管真空3.7×10^-5 Pa、二极管电压1.95 MV、脉宽120 ns（FWHM）、阴极温度1 120 ℃时,获得最大收集电流1 038 A,发射电流密度约13 A/cm²。实验结果表明,工作状态下阴极发射能力与激活温度、系统真空度关系密切。