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首页> 外文期刊>Physica Scripta: An International Journal for Experimental and Theoretical Physics >Parametric excitation of surface electron cyclotron O-modes by an external alternating electric field
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Parametric excitation of surface electron cyclotron O-modes by an external alternating electric field

机译:外部交变电场对表面电子回旋加速器O型的参量激发

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Using the model of uniform semi-bounded plasma, it is shown that the influence of an external alternating electric field in the range of electron cyclotron frequencies leads to excitation of eigen ordinary polarized waves at the first harmonic of electron cyclotron frequency. The external electric field was assumed to be uniform and monochromatic; electro-dynamical properties of the plasma were described by the kinetic Vlasov-Boltzmann equation in the approach of a weak spatial dispersion of plasma. Two components of these modes' wave vector oriented across an external magnetic field are taken into consideration. Fields of these electron cyclotron O-modes are described by the Maxwell equations; their phase velocity is assumed to be less than the velocity of light. Nonlinear boundary condition-described discontinuity of the modes' tangential magnetic field is formulated using the concept of a nonlinear surface electric current. The infinite set of equations for harmonics of these O-modes' tangential electric field has been derived with the aid of this nonlinear boundary condition. It is solved using a wave packet consisting of the basic harmonic and two nearest satellite harmonics. A simple analytical expression for growth rates of these surface waves' parametric instability is obtained; the influence of plasma parameters on their excitation is numerically analyzed.
机译:使用均匀的半边界等离子体模型,表明在电子回旋频率范围内,外部交变电场的影响导致在电子回旋频率的一次谐波处激发本征普通极化波。假定外部电场是均匀且单色的。等离子体的电动力学性质通过动力学Vlasov-Boltzmann方程在等离子体弱空间弥散的方法中描述。考虑了这些模式的波矢量在外部磁场中的两个分量。这些电子回旋加速器O模的场由麦克斯韦方程描述。假定它们的相速度小于光速。非线性边界条件所描述的模式切向磁场的不连续性是使用非线性表面电流的概念来表述的。借助于这种非线性边界条件,已经导出了这些O型切向电场的谐波的无限等式组。它是通过一个由基本谐波和两个最近的卫星谐波组成的波包来解决的。获得了这些表面波的参数不稳定性增长率的简单解析表达式;数值分析了等离子体参数对其激发的影响。

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