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Excitation of Electromagnetic Wake Fields by one-dimensional Electron Bunch in Plasma in the Presence of Circularly Polarized Intense Electromagnetic Wave

机译:用一维电子激发电磁尾迹场   在圆极化激烈的存在下在等离子体中束   电磁波

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摘要

The excitation of electromagnetic (EM) wake waves in electron plasma by anone-dimensional bunch of charged particles has been considered in the presenceof intense monochromatic circularly polarized electromagnetic (CPEM) pump wave.In the zero state (in the absence of bunch) the interaction of the pump wavewith plasma is described by means of Maxwell equations and relativisticnonlinear hydrodynamic equations of cold plasma. The excitation of linear wavesby one-dimensional bunch is considered on this background. It is shown thatthere are three types of solutions of linear equations obtained for inducedwaves corresponding to three ranges of parameter values of the pump wave, bunchand plasma. In the first range of parameter values the amplitude of transversecomponents of induced waves is shown to grow as the bunch energy and after somevalue of the relativistic factor of the bunch to be almost independent of theenergy and increase proportional to the intensity and frequency of the pumpwave. The dependence of longitudinal component of induced waves on therelativistic factor of the bunch is weak. Its amplitude and wavelength grow asthe intensity of pump wave. The second range of parameters is a resonance one.The amplitude of the wave excited by the bunch is a linear function of thedistance to the bunch. In the third range of parameter values the longitudinalcomponent of induced fields are localized near the bunch boundaries and areexponentially decreased with the increase in distance from these boundaries.The amplitudes of transverse components of induced waves reach a constant valuewith the distance from the bunch boundaries.
机译:在强单色圆极化电磁(CPEM)泵浦波的存在下,曾考虑过一维束带​​电粒子在电子等离子体中激发电磁(EM)尾波。在零态(没有束)下,相互作用用麦克斯韦方程和冷等离子体的相对论非线性流体力学方程描述了泵浦等离子体的波场。在此背景下考虑了由一维束激发线性波。结果表明,对于感应波,存在对应于泵浦波,束流和等离子体的三个参数值范围的三种线性方程解。在参数值的第一个范围中,感应波的横向分量的振幅显示为随着束能量的增加而增加,并且在束的相对论因子的某个值之后几乎与能量无关,并且与泵浦波的强度和频率成比例地增加。感应波的纵向分量对束的相对论因子的依赖性很弱。其幅度和波长随着泵浦波的强度而增长。参数的第二个范围是共振。束激发的波的幅度是到束的距离的线性函数。在参数值的第三个范围内,感应场的纵向分量位于束边界附近,并且随着与这些边界的距离增加而呈指数下降。感应波的横向分量的振幅随着距束边界的距离而达到一个恒定值。

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  • 年度 1999
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  • 正文语种 {"code":"en","name":"English","id":9}
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