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Studies of three‐cylinder electrostatic mirrors and lenses

机译:三缸静电反射镜和透镜的研究

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With the aim of using it in mass spectrometry, we have tried to find an axisymmetric electrostatic system with very particular characteristics, viz. reduced spherical and chromatic aberrations. We chose a system made up of three coaxial cylinders of radius ρ. The inner electrode is 0.90 ρ long and is separated from the outer cylinders (which are taken to be of infinite length) by two identical gaps of 0.40 ρ. This system has been studied from both the mirror and the lens point of view. The mirror is studied using two electrostatic parameters. The potentials of the three cylinders are reffered to as V1, V2, and V3. The first parameter used is Rd=100 (V1-V2)/(V1-V3) and the second is V3/V1. For six values of Rd, ranging from 100 to 74, we examine the paraxial characteristics and the coefficients of spherical and chromatic aberration as a function of V3/V1. We only deal with the area where the mirrors are convergent and where the radii of curvature do not exceed 10ρ. For the values of Rd studied, other than 100, we use a field of variation from -0.10 to -0.50 for V3/V1. When we study the lens, we deal with the area where the outer potentials V1 and V3 are identical. There is thus only one variable, the ratio V2/V1 of the potentials of the first two cylinders. We consider two cases: V2/V1≳1 and V2/V1≪1. Among the results obtained, we have chosen two groups of mirrors for which the chromatic aberration coefficient Cc is null and whose radii of curvature are greater than 6.60 ρ, a group of mirrors for which the spherical aberration coefficient Cs is null and where Cc is greatly reduced (here the radii of curvature are greater than-n 4.00 ρ), and a mirror for which both Cc and Cs are null and which has a radius of curvature of 7.28 ρ.
机译:为了在质谱中使用它,我们试图找到一种具有非常特殊特性的轴对称静电系统,即。降低球差和色差。我们选择了一个由三个半径为ρ的同轴圆柱体组成的系统。内电极的长度为0.90ρ,与外圆柱(被认为是无限长的)之间有两个相同的0.40ρ的间隙。已经从反射镜和透镜的角度研究了该系统。使用两个静电参数研究反射镜。三个圆柱的电势分别为V1,V2和V3。使用的第一个参数是Rd = 100(V1-V2)/(V1-V3),第二个参数是V3 / V1。对于从100到74的六个Rd值,我们检查了近轴特性以及球差和色差系数与V3 / V1的关系。我们仅处理反射镜会聚且曲率半径不超过10ρ的区域。对于研究的Rd值(不是100),对于V3 / V1,我们使用从-0.10到-0.50的变化范围。在研究透镜时,我们要处理的是外部电位V1和V3相同的区域。因此只有一个变量,即前两个圆柱的电势之比V2 / V1。我们考虑两种情况:V2 /V1≳1和V2 / V1≪1。在获得的结果中,我们选择了两组色差系数Cc为零且曲率半径大于6.60ρ的镜子,一组球面像差系数Cs为零且Cc很大的镜子。反射镜(此处的曲率半径大于-n 4.00ρ),并且反射镜的Cc和Cs均为零,且曲率半径为7.28ρ。

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    《Journal of Applied Physics 》 |1982年第6期| P.3950-3956| 共7页
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  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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