非均匀磁场约束条件下的电子束空气等离子体特性

为了揭示大气环境电子束等离子体的性质,基于蒙特卡罗程序包Geant4建立了一个包含电离、激发以及轫致辐射等物理过程的计算模型,用于模拟非均匀磁场约束条件下高能强流稳态电子束的输运特性、以及大气环境等离子体的性质。结果表明:非均匀磁场可以有效控制电子束在空气中的输运轨迹,显著降低电子束的发散;随着电子束在空气中行程的增加,电子束能谱开始展宽并向低能区移动;输运装置出口能量损失比电子束射程末端高2个量级,且随着电子束输运距离的增加,等离子体密度降低;等离子体密度的高低与电子束能量直接相关。     

托卡马克电场电子注入的漂移电子束研究

 研究了漂移电子束中电子的运动规律, 得到了电子在外加电场、纵磁场和电子束自场中的运动轨迹和漂移速度表达式, 并就它们的成束条件、成束形状和电压要求以及束的稳定性条件进行了比较和讨论, 认为阴极垂直于纵磁场放置更好一些。     

高阶Chen-Lee-Liu方程在半直线上的初边值问题

该文运用Fokas方法分析了高阶Chen-Lee-Liu方程在半直线上的初边值问题,证明了高阶Chen-Lee-Liu方程初边值问题的解可以用复λ平面上的矩阵Riemann-Hilbert问题的形式解唯一表示.     

Electron beam density imaging system at Beam study using a portable slit the Shanghai Electron Ion Trap

In this work, a portable slit imaging system is developed to study both the electron beam diameter and the profile of the newly developed Shanghai Electron Beam Ion Trap （Shanghai EBIT）. Images are detected by a charge coupled device （CCD） sensitive to both X rays and longer wavelength photons （up to visible）. Large scale ray tracings were conducted for correcting the image broadening effects caused by the finite slit width and the finite width of the CCD pixels. A numerical de-convolution method was developed to analyse and reconstruct the electron beam density distribution in the EBIT. As an example of the measured beam diameter and current density, the FWHM （full width at half maximum） diameter of the electron beam at 81 keV and 120 mA is found to be 76.2 μm and the density 2.00 × 10^3 A.cm-2, under a magnetic field of 3 T, including all corrections.     

圆形有界磁场问题的分类及解析

1对心飞入问题【例1】(2002年高考天津卷)电视机的显像管中,电子束的偏转是用磁偏转技术实现的.电子束经过电压为U的加速电场后,进入一圆形匀强磁场区,如图1所示.磁场方向垂直于圆面.磁场区的中心为O,半径为r.当不加磁场时,电子束将通过O点而打     

High-Precision Calibration of Electron Beam Energy from the Hefei Light Source Using Spin Resonant Depolarization

Electron beam in high-energy circular accelerator was found to spontaneously become transverse polar- ization by emitting spin-flip synchrotron radiation. It opens the possibility for accurate measurement of the average beam energy in the storage ring. Due to the fact that the average spin tune Us （the number of spin precession per orbital revolution） is proportional to the average beam energy E.     

用电子束电磁偏转原理测电阻值的研究

传统的伏安法测电阻实验中无论采取电流表内接法还是外接法,都会由于电表内阻的存在,使得测量结果产生误差.本文尝试用电子束测试仪取代实验中的电压表位置实现完全断路,并设计实验步骤对电阻值进行测量,经过数据的比对,发现测量结果的相对误差较小,从而实现借助力学量来测电学量.     

一种大入射角容差宽带薄膜偏振器

通过组合长波通和短波通膜堆的方法,设计并制备了一种大入射角容差宽带薄膜偏振器。该薄膜为HfO_2/SiO_2结构,采用无离子束辅助的电子束蒸发工艺,蒸发金属铪和SiO_2制得。对该膜的透射率光谱、激光损伤阈值和形貌进行了研究,结果显示其不仅在1044~1084 nm波段内都具有很高的对比度,而且在1064 nm波长、53°~60°的入射角范围内具有很大的消光比和激光损伤阈值,且损伤特性基本不随入射角变化。该偏振器的P光损伤阈值约为20 J/cm~2,损伤主要由基板与薄膜界面处的纳米级缺陷所引起;S光损伤阈值约为45 J/cm~2,损伤主要由激光辐照下薄膜表面的等离子烧蚀现象引起。     

Study of a compact external magnetic field radial split-cavity oscillator

With the experiment result analyses of a coaxial virtual cathode oscillator (CVCO), a new kind of compact radial split cavity oscillator (RSCO) is presented in this paper. On the oscillator, a low resistance tube is formed by using the diode structure of a CVCO, and a radial split-cavity structure is formed by several meshes that cause the electronic beam to transmit. Calculating all kinds of parameter, at the input parameter 350 kV, 27 kA, the numerical simulation results show that the average output microwave power is about 4.0 GW, the microwave frequency is 1.37 GHz, and the electronic efficiency is 42.3%.     

Simulation and analysis of the transverse spectrum in HIRFL-CSR

Particles in a storage ring oscillate in the longitudinal and transverse dimensions. Therefore, the signal that beam has generated can be analyzed in the frequency domain to extract many beam parameters, such as tune, momentum spread, emittance and their evolution with time and so on. In this paper, the transverse spectrum in HIRFL-CSR was simulated and analyzed under different conditions, including electron cooling, hollow electron beam, solenoid effect, the tune shift caused by power supply ripple and the misalignment between ion and electron beams. The result of the simulation shows that the longitudinal magnetic field of the electron cooling device should be compensated by a “compensation solenoid”, and the power supply ripple must be controlled, otherwise the accumulation would be affected and the beam would be lost.