EAST-NBI磁偏转系统束传输特性模拟研究

根据EAST-NBI偏转系统工作原理,分析了束流在偏转系统传输的基本过程和特点。利用直接蒙特卡罗方法,发展了中性束注入器束偏转区域束流传输模拟程序。结果显示:EAST-NBI磁偏转系统可很好地剥离束流中的剩余离子;束偏转区域束流再电离损失约为2.43%;束流180°偏转所带来线聚焦过程使偏转磁体磁极护板局部面临较高的热流密度。     

一种新的消色差等时性磁偏转系统

描述了一种新的消色差等时性磁偏转系统．它由二个反对称的预偏磁铁和一个主偏磁铁构成。根据六维传输矩阵导出了系统的消色差和等时性关系式．该系统具有优良的消色差性、等时性和良好的聚焦特性。这种结构紧凑的三磁铁偏转系统适用于自由电子激光器的束流传输。     

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According to the design parameters of 5MW-NBI beam line of HL-2M tokamak, spatial arrangement of components, geometrical focus characters and so on, 3D model of the deflecting magnet with 8 groups of wires is built up. With an electromagnetic field simulation software-CST Studio, the deflection magnetic field distribution and deflection trajectories of ion beams with different components are obtained. With the simulation results the physical structure of deflecting magnet is optimized, the engineering design of the magnet is completed and then the manufacture and test are finished. The testing result of the magnetic field distribution of the deflecting magnet shows: the error between measurement value and calculation result is less than ±5%, and the machined deflecting magnet can meet the design requirement.     

HL-2M装置5MW-NBI加热束线偏转磁体研制

根据HL-2M装置5MW-NBI加热束线总体设计参数、注入器的部件空间布局、几何汇聚特点等,建立了基于8饼线圈的注入器偏转磁体3D模型。利用电磁场模拟软件CST Studio详细模拟了注入器的偏转磁体产生的偏转磁场分布,不同成份离子束的偏转轨迹。在模拟分析结果的基础上优化了偏转磁体的物理结构,完成了磁体的工程设计、加工和测试。偏转磁体的磁场测试结果表明,测试值与CST计算值的偏差小于±5%,达到注入器偏转磁体设计要求。     

Design and development of the 6–18 MeV electron beam system for medical and other applications

A system for the electron and photon therapy has been designed and developed at SAMEER, IITB, Mumbai. All the components of the system such as the 270° beam bending electromagnet, trim coils, magnet chamber, electron scattering foil, slits, applicators, etc., were designed and fabricated indigenously. The electrons of 6, 8, 9, 12, 15 and 18?MeV energies were provided by a linear accelerator, indigenously designed and made at SAMEER, IITB campus, Mumbai. The electron beam from the LINAC enters the magnet chamber horizontally, and after deflection and focusing in the 270° bending magnet, comes out of the exit port, and travels a straight path vertically down. After passing through the beryllium and tantalum scattering foils, the electron beam gets scattered and turns into a solid cone shape such that the diameter increases with the travel distance. The simulation results indicate that at the exit port of the 270° beam bending magnet, the electron beam has a divergence angle of ≤ 3?mrad and diameter ～2–3?mm, and remains constant over 6–18?MeV. Normally, 6–18?MeV electrons are used for the electron therapy of skin and malignant cancer near the skin surface. On a plane at a distance of 100?cm from the scattering foils, the size of the electron beam could be varied from 10?cm?×?10?cm to 25?cm?×?25?cm using suitable applicators and slits. Different types of applicators were therefore designed and fabricated to provide required beam profile and dose of electrons to a patient. The 6?MeV cyclic electron accelerator called Race-Track Microtron of S. P. Pune University, Pune, was extensively used for studying the performances of the scattering foils, electron beam uniformity and radiation dose measurement. Different types of thermoluminescent dosimetry dosimeters were developed to measure dose in the range of 1–10kGy.     

消色散270°偏转磁铁系统设计及束流动力学研究

对三种常用结构的270°偏转磁铁进行系统的分析研究,采用数值计算和模拟方法对双磁铁不对称偏转结构、三块90°磁铁偏转结构和70°+130°+70°偏转结构这三种不同的270°偏转磁铁系统进行模拟,给出偏转系统的消色散传输条件,并且分析了束流包络在偏转系统和出口管道中的变化情况。经过分析对比,详细列出了三种结构的优势与劣势。双磁铁不对称结构适用于医用加速器,三块90°磁铁偏转结构适用于需要在出口长距离漂移的辐照加速器,而70°+130°+70°偏转结构可以满足出口一定距离的无损漂移,同时实现相对较低的成本,是工业辐照加速器较为经济适宜的选择。     

Design of magnet and control of the beam emittance for Penning H- ion source

The design requirement and principle of the deflection magnet for Magnetron and Penning H- ion source are discussed.It is proved that there exists a maximum emittance for the beam that may be transformed by the magnet into a state with equal Twiss parameters of αr=αy and βr =βy,which is the requisite condition to get a minimum emittance at the entrance of RFQ after transporting by a LEBT with solenoids.For this maximum emittance,the corresponding magnetic field gradient index is 1.     

A plastic scintillating fiber position detector in vacuum for the test beam facility at BEPCⅡ-LINAC

Two plastic scintillating fiber position detectors for charged particles have been designed, built and installed inside the vacuum tube near two sides of the DM2 deflection magnet on the E3 beam line of the test beam facility at the BEPC-LINAC. A one-dimensional position resolution of sim 1 mm with a sensitive area of 60 mm×60 mm has been obtained for this detector.     

A plastic scintillating fiber position detector in vacuum for the test beam facility at BEPCⅡ-LINAC

Two plastic scintillating fiber position detectors for charged particles have been designed, built and installed inside the vacuum tube near two sides of the DM2 deflection magnet on the E3 beam line of the test beam facility at the BEPC-LINAC. A one-dimensional position resolution of sim 1 mm with a sensitive area of 60 mm×60 mm has been obtained for this detector.     

基于磁化电流法的双稳压电悬臂梁磁力精确分析

双稳压电悬臂梁结构常常用于振动能量采集系统,其中的非线性磁力与系统势函数和动力学方程的建立紧密相关,非线性磁力的正确分析和精确计算对系统振动响应和能量采集效果的准确预测至关重要.本文采用形状函数分析方法,通过悬臂梁弯曲斜率的整体积分计算,得到了悬臂梁末端的运动轨迹及其末端磁铁精确的位置与姿态,并由此根据磁化电流理论建立了双稳压电悬臂梁能量采集系统的磁力计算模型,给出了末端磁铁受到的水平轴向磁力和竖直纵向磁力及其合磁力的变化规律.数值模拟发现,随着末端磁铁竖直纵向位移逐渐增大,磁铁受到的水平轴向磁力和竖直纵向磁力都会依次由排斥力转变为吸引力,从而导致磁力合力的方向会随磁铁位移发生跨越两个象限的大幅度变化.实验验证表明,磁力计算结果与实验测量结果符合良好,其精确度优于现有文献方法的精度,因此本文的方法可以准确预测双稳压电悬臂梁振动过程的磁力变化规律.     

Measurement of azimuthal magnetic fields in a Z-pinch gas discharge using the faraday rotation of a probe beam

The Faraday rotation of the plane of polarisation of a probe beam by azimuthal magnetic fields in the presence of beam deflection caused by refractive index gradients is discussed for a plasma carrying an axial current. A method for calculation of the magnetic field profile from experimental data is described. Bθ can be found by Abel inversion if the electron density is known and if deflected rays can be collected by an optical system and focussed onto a detector. Typical Faraday rotations calculated for the Bennett pinch assuming small beam deflection are found to be proportional to the plasma current and to the angle of deflection. If the probe beam wavelength is chosen to satisfy the approximate relation N₀λ² ≈ 3.5 × 10¹³ m^-1, where N₀ is the electron density on the axis, measurement of Bθ with beam deflections less than 2 × 10^-2 radians should be possible in cases where small rotations can be detected in the mid-to-far infra-red part of the spectrum.     

基于PID算法的磁场闭环控制技术研究

已有的束流磁场控制方法大多采用开环的方式,即根据磁场需求直接设置磁铁电源输出的电流或电压值.但开环状态的磁场在现场噪声以及磁铁自身涡流效应的影响下,极容易发生偏移.针对此问题,设计了基于PID算法的磁场闭环控制系统.该系统以偏转磁铁为控制对象,使用霍尔传感器获取磁场值作为反馈,磁铁电源励磁电流的输出作为控制系统的输入量...     

Experimental evaluation of the gas-phase collision cross-section of effusive Au beam with noble gases: The effect of size and flux

We find that the effusive atomic beam of Au atoms is deflected away by collision with noble gas atoms crossing in a perpendicular geometry with a beam flux of >1 × 10¹⁶/cm²s. The ratio of defected Au atoms is found to increase proportional to the flux of noble gases. In addition, the effective cross-section for the collision between Au and noble gases (Ne, Ar, Xe) is measured to increase in an order of Ne < Ar < Xe. As a result of the increased collision probability, the deflection ratio of Au beam in the noble gases is measured to be enhanced for the Au flux in the range of 1 × 10¹¹–10¹³ Au/cm²s. Our results show that the gas-phase collision can be reliably determined by measuring the deflection ratio. The experimentally determined collision cross-section also explains the variation in the deflection ratio among various noble gases and the importance of a long-range van der Waals interaction between Au and noble gases in the deflection efficiency.     

A new rectangular beam theory

A new theory for beams of rectangular cross-section which includes warping of the cross-sections is presented in the present work. By satisfying the shear-free conditions on the lateral surfaces of the beam a pair of coupled equations of motion are obtained such that no arbitrary shear coefficient is required. It is shown that the uncoupled equation for the transverse displacement is the same as the corresponding equation in Timoshenko beam theory provided that for the Timoshenko equation the shear coefficient is taken to be $\text{5}\text{6}$; this value lies within the range of values, 0·822–0·870, appearing in the literature for the beam of rectangular cross-section. Results for two typical static examples are given for both the new theory and Timoshenko beam theory. These results are compared with the solutions of the comparable problems in the linear theory of elasticity. For the end loaded cantilever beam the new theory predicts the same result for the neutral surface deflection as does the linear theory of elasticity while Timoshenko beam theory underestimates the shear correction term by 20%. For the uniformly loaded and simply supported case both beam theories provide the same overestimate of the central deflection when compared with the theory of elasticity solution.     

通过极化原子束的磁偏转实现激光同位素浓缩

本文描述一种通过极化原子束的磁偏转实现同位素和同质异能素浓缩的新方法。用具有不同频率和偏振的激光进行选择性光抽运,使束中两同位素的原子分别反向高度极化,然后使这些反向极化的原子在经过自旋选态磁铁后沿不同方向偏转,从而实现同位素浓缩。推算了此法的选择性和产量,与其他方法相比,讨论了其优缺点和可能的应用前景。提出了用锂或钾进行实验的方案。 关键词：     

Spin-rotating magnet for the ΔσL(np) experiment at LHEP JINR

The spin rotating magnet (SRM) is purposed for the orientation rotation of the nucleon spins in the polarized beam from the transverse (T) direction with respect to the nucleon beam momentum to the longitudinal (L) one. The longitudinally polarized neutron beam was used in the experiment for measuring the total cross section difference Δσ_L(np) with parallel and antiparallel orientation of the participant L polarization. To perform the nucleon spin rotation in the polarized nucleon beam through the angle of 90° over the beam momentum region of ～1.8–5.5 GeV/c, a proper spin rotation device had to be prepared. For this purpose, the necessary calculations of corresponding values of the magnetic induction integral were carried out. Using the calculations the dipole magnet SP 57 type was chosen for the Δσ_L(np) experiment and the required reconstruction of its pole tips was also accomplished. After the SRM installation at the neutron beam line the appropriate apparatus set for the magnetic measurements was prepared and the precise measurements of the whole set of the SRM characteristics were performed. The obtained results for the SRM magnetic field parameters were successfully used during the Δσ_L(np) experimental runs to specify the current at this magnet coil corresponding to the calculated magnetic induction integral for the given neutron beam momentum.     

Magnetically actuated bi-directional microactuators with permalloy and Fe/Pt hard magnet

Bi-directional polyimide (PI) electromagnetic microactuator with different geometries are designed, fabricated and tested. Fabrication of the electromagnetic microactuator consists of 10 μm thick Ni/Fe (80/20) permalloy deposition on the PI diaphragm by electroplating, high aspect ratio electroplating of copper planar coil with 10 μm in thickness, bulk micromachining, and excimer laser selective ablation. They were fabricated by a novel concept avoiding the etching selectivity and residual stress problems during wafer etching. A mathematical model is created by ANSYS software to analyze the microactuator. The external magnetic field intensity (H_ext) generated by the planar coil is simulated by ANSYS software. ANSYS software is used to predict the deflection angle of the microactuator. Besides, to provide bi-directional and large deflection angle of microactuator, hard magnet Fe/Pt is deposited at a low temperature of 300 °C by sputtering onto the PI diaphragm to produce a perpendicular magnetic anisotropic field. This magnetic field can enhance the interaction with H_ext to induce attractive and repulsive bi-directional force to provide large displacement. The results of magnetic microactuator with and without hard magnets are compared and discussed. The preliminary result reveals that the electromagnetic microactuator with hard magnet shows a greater deflection angle than that without one.     

电扫描型单缝单丝强流离子束发射度测量仪

 介绍了一台基于电偏转扫描方法的强流离子束发射度仪,讨论了发射度仪硬件的系统构成和设计要点,该发射度仪采用阶梯型电压对通过前缝的束流进行扫描来获得束流散角信息。并对测量计算软件和数据处理方法进行了介绍,采用了先扣除本底,再设置阈值的方法进行数据处理。处理后的数据利用程序可获得均方根和边界发射度、束斑大小、最大正负散角以及发射度相图。利用该发射度仪对ECR离子源引出的强流质子束的发射度进行了测量,并对测量数据进行了分析。对于引出电压为50 kV、脉冲重复频率为166 Hz、脉冲宽度为1 ms、平均束流强度为4 mA的质子脉冲束,其归一化均方根发射度为0.27 pmm·mrad。     

黑腔中高斯型激光束偏折的模拟研究

利用三维激光等离子体相互作用流体程序LAP3D数值模拟研究了高斯光束在均匀等离子体传播过程中的激光束偏折现象,分别考察了激光强度变化和等离子体横向流的流速变化对束偏折的影响。模拟结果表明:当流速接近离子声速时,激光束偏折效应最明显,此时激光偏折程度与激光强度成正比;当流速逐渐小于离子声速时,激光束偏折行为受抑制逐渐减弱;而当流速逐渐大于离子声速时,激光光强包络的变化以衍射效应为主。     

Deflection of an electron beam with a 1.8-MeV energy incident at glancing angles on a dielectric surface

The first results of investigations into the effect of self-deviation of an electron beam with intermediate energy by a dielectric surface, previously discovered by the authors for the interaction of electrons with a glass surface, are presented in the paper. It is shown that optimizing the deflection process and choosing a dielectric target, angles of beam deflection of the order of 5–8° can be obtained and stabilized during subsequent irradiation of the target, which is especially important for applications of this effect to electron-beam optics. Scientific Research Institute of Nuclear Physics at Tomsk Polytechnic University. Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 9, pp. 12–17, September, 1999.