电子束-波相互作用理论的新途径

L. Shenggang, Y.Y. Wei, Yan Yang, R. J. Barker
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摘要

本文提出了一种新的研究任意射频结构中电子束与波相互作用的理论方法。在任何这样的相互作用系统中,都有两个坐标系:实验室坐标系;等离子体的静止坐标系,如果存在的话;以及电子束的运动坐标系。电子束和等离子体都被认为是具有不同特性的特殊介质。介电常数张量和磁导率张量可以在运动坐标系中找到,而等离子体的介电常数张量可以在实验室坐标系中找到。然后,利用电磁场在闵可夫斯基空间中的变换和四维波矢量的洛伦兹变换,将运动坐标系中的物理量全部转换到实验室坐标系中。然后利用带有传递本构张量的麦克斯韦方程组来推导所需的色散方程。这种新方法是研究电子束-波相互作用的一种非常有效和精确的方法。
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A new approach for the theory on electron beam-wave interactions
A new approach to the theoretical study of the electron beam-wave interaction in arbitrary RF structures is presented in this paper. In any such interaction system, there are two coordinate systems: the lab system; the rest coordinate system for the plasma, if it exists; and the moving coordinate system for the electron beam. Both the electron beam and the plasma are considered special media with different characteristics. The permittivity tensor and the permeability tensor can be found in the moving coordinate system for the beam while that for the plasma can be found in the lab coordinate system. Then, making use of the transformation of electromagnetic fields in Minkovski space and the Lorentz transformation of the 4D wave vectors, all the physics quantities in the moving coordinate system can be transferred into the lab coordinate system. Then the Maxwell's equations with the transferred constitutive tensors should be used to derive the desired dispersion equation. This new approach is a very efficient and accurate method for the study of electron beam-wave interactions.
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