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中子应力谱仪常用聚焦单色器的模拟与比较 总被引:1,自引:0,他引:1
用蒙特卡罗中子射线追踪程序McStas对中子衍射应力谱仪单色器部件进行模拟优化:以Cu(220)比较了单色器起飞角和准直系统对样品处中子注量率、分辨率的影响;计算得到给定条件下单色器最佳单晶条数和镶嵌度;单晶条倾角精度建议好于0.1°;计算了Cu(222)、(220)和(002)在不同起飞角情况下获得的中子注量率;相同条件下,Cu和Ge常用晶体单色器中以Cu(220)获得的中子注量率最大,而Cu(222)获得的波长分辨率最佳。 相似文献
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为提高样品处入射中子束强度,满足高分辨和小体积标样测量的需要,应用MCSTAS软件对中国先进研究堆上应力测量中子衍射谱仪的核心部件垂直聚焦单色器进行模拟和优化设计,得到了单色器在不同起飞角下的最佳聚焦条件,即所需的曲率半径和相邻单晶条之间的最佳倾角。在此条件下,可获得相对于平板单色器6~7倍的强度增益,样品处中子注量率达107cm-2•s-1以上。在使用聚焦单色器的情形下,对标准的α-Fe多晶样品在无应变、拉应变和压应变下的(211)衍射峰进行了模拟。结果表明:该谱仪的分辨水平至少能测量500με以上的应变,且应变测量最高精度约为20με。 相似文献
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为研究单色器对中子能谱的选择规律,本文利用MCSTAS程序模拟分析了机械速度选择器与晶体单色器几个特征参数对中子能量选择影响。分析结果显示经机械速度选择器单色选择中子注量率要下降1~2个量级,而晶体单色器要下降2~3个量级。因此,对于单色化要求比较高选用晶体单色器,对于实验时间要求较高的选用机械速度选择器。 相似文献
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A. D. Vlasov 《Atomic Energy》1956,1(5):687-694
A linear theory for alternating-gradient (strong) focusing in linear ion accelerators is presented.Presented at the All-Union Conference on the Physics of High Energy Particles, May 18, 1956. 相似文献
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C. L. Olson 《Journal of Fusion Energy》1981,1(4):309-339
Inertial confinement fusion with ion beams requires the efficient delivery of high energy (1 MJ), high power (100 TW) ion beams to a small fusion target. The propagation and focusing of such beams is the subject of this paper. Fundamental constraints on ion beam propagation and focusing are discussed, and ion beam propagation modes are categorized. For light ion fusion (LIF), large currents (2–33 MA) of moderate energy (3–50 MeV) ions of low atomic number (1A12) must be directed to a target of radius 1 cm. The development of pulsed power ion diodes for LIF is discussed, and the necessity for virtually complete charge neutralization during transport and focusing is emphasized. Fornear-term LIF experiments, the goal is to produce pellet ignition without the standoff needed for the ultimate reactor application. Ion diodes for use on Sandia National Laboratories Particle Beam Fusion Accelerators PBFA-I (2–4 MV, 1 MJ, 30 TW, operational) and PBFA-II (2–16 MV, 3.5 MJ, 100 TW, scheduled for operation in 1985) are discussed. Ion beam transport from these diodes to the pellet is examined in reference to the power brightness . While values of =2–5 TW/cm2/sr have been achieved to date, a value of 100 TW/cm2/sr is needed for breakeven. Research is now directed toward increasing , and means already exist (e.g., scaling to higher voltages, enhanced ion diode current densities, and bunching), which indicate that the required goal should be attainable. Forfar-term LIF applications, the goal is to produce net energy gain with standoff suitable for a reactor. This may be achieved by ion beam transport in preformed, current-carrying plasma channels. Channel transport research is discussed, including experiments with wire-initiated, wall-initiated, and laser-initiated discharge channels, all of which have demonstrated transport with high efficiency (50–100%). Alternate approaches to LIF are also discussed, including comoving electron beam schemes and a neutralized beam scheme. For heavy ion fusion (HIF), moderate currents (10 kA) of high energy (10 GeV) ions of high atomic number (A200) must be directed to a target of radius 0.3 cm. Conventional accelerator drivers for HIF are noted. For a baseline HIF reactor system, the optimum transport mode for low charge state beams is ballistic transport in near vacuum (10–4–10–3 Torr lithium), although a host of other possibilities exists. Development of transport modes suitable for higher charge state HIF beams may ultimately result in more economical HIF accelerator schemes. Alternate approaches to HIF are also discussed which involve collective effects accelerators. The status of the various ion beam transport and focusing modes for LIF and HIF are summarized, and the directions of future research are indicated. 相似文献
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Alexander D. Dymnikov Genoveva Martínez 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》1997,130(1-4):74-79
This paper investigates the possibility of utilising an electrostatic multiple cylinder lens to focus the beam in microprobes. Multiple cylinders reduce the lens potentials which are required. We use a new analytical model of the axial potential distribution varying the parameters of this distribution and the size of the object and aperture diaphragms to obtain the minimum spot size at the specimen for a given beam emittance and finding by this way the optimal parameters of the axial potential distribution. For synthesising the optimal physical model we applied an accurate version of the Integral Equation Method to solve Laplace's equation in order to obtain the parameters of the physical model which has the same axial potential distribution as the optimal analytical model. 相似文献
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In this paper we consider the use of strong focusing in linear proton accelerators and carry out a detailed quantitative analysis of the motion of protons in the system. Design calculations for quadrupole lenses are given together with the experimental results obtained with the use of strong focusing in a 5.5 Mev linear proton accelerator.In conclusion the authors wish to take this opportunity to thank Acid. AN SSSR K. D. Sinel'nikov and Cand. Phys.-Math. Sci. Ya. B. fainberg for their continued interest in this work and for valuable discussions. 相似文献