带可扩展滤网的扇形滤波器的设计

I. Spivak-Lavrov, S. Sharipov, A.B. Seiten, A.A. Trubitsyn
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摘要

偏转板由两块平行的导电板组成,可产生偏转电场。它们可用于控制带电粒子(电子或离子)的流动。偏转板的еdgе fiеld效应会导致带电粒子在纵向和横向的速度发生变化,从而使它们的实际轨迹发生变化,偏离理想轨迹,这就违反了使用它们的体视光学设备的时空分辨率。除此之外,偏转板输入端的电场也会随时间而变化,在偏转板偏转带电粒子束时也必须考虑到这一点。因此,在许多情况下,使用两端开口的偏转板是不合适的,因为这样会形成不可控的散射场。在本文中,我们可以考虑在偏转板的输出端使用带有扩展屏幕的偏转板场,这样就可以在偏转板的输出端使用偏转带电粒子束。利用复变函数理论的方法,得到了带接地屏的导流板边缘场的解析表达式。首先,通过将屏幕接地,屏蔽偏转板的偏转场,我们可以将边缘电场局部化,减少不受控制的散射场;其次,这样的场可以通过解析精确计算出来。
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Еdgе fiеld of dеflеctorplаtes with expanding screens
Deflector plates consist of two parallel conductive plates that create a deflecting electric field. They can be used to control the flow of charged particles ― electrons or ions. The effect of the еdgе fiеld of deflector plates leads to a change in the velocity of charged particles in the longitudinal and transverse directions, consequently of which their real trajectories change, deviating from ideal ones, which violates the space-time resolution of corpuscular optical devices in which they are used. Apart from that, the electric field at the input to the plates of deflector can vary over time, which must also be taken into account when the deflector diverts the beam of charged particles. Thus, in many cases, the use of deflector plates with open ends is inappropriate, since uncontrolled scattering fields are formed. In this article, we can consider the field of deflector plates with expanded screens at the output, so that deflecting beams of charged particles can be used at the output of deflector plates. Using the methods of the theory of complex variable functions, analytical expressions for the edge field of deflector plates with grounded screens were obtained. Firstly, by grounding the screens and shielding the plates from the deflection field, we can localize the edge electric field and reduce the uncontrolled scattering fields, and secondly, such a field can be accurately calculated analytically.
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