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Spectrum broadening and degradation of the O-X mode coupling efficiency due scattering of a microwave beam on plasma density fluctuations

机译:微波光束对等离子体密度波动的频谱扩展和劣化耦合施加效率

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Linear transformation of the ordinary (O) and extraordinary (X) electromagnetic modes in the vicinity of the plasma cutoffs in magnetized plasma is a basis for advanced schemes of microwave heating and diagnostic of overdense plasmas (where the central density exceeds the cutoff) in magnetic fusion research. A significant influence of density fluctuations, inherent of hot magnetized plasma in toroidal magnetic traps, on the process of linear transformation was first noted in [1], where a simple phenomenological model of this phenomenon was considered. Recently, by a more rigorous analysis, this picture has been substantially revised [2]. As a result of solving the truncated Maxwell equations in the linear interaction region in the presence of density fluctuations, it was established that the dominant effect in the O-X coupling efficiency is due to the small-angle scattering of the wave beam on the fluctuations along the propagation path towards the cutoff, at least fluctuations for the parameter range corresponding to modern experiments. Outside the coupling region, the scattering modifies the incident O-wave beam, which affects its subsequent transformation and reflection. At this, the so-called enhanced scattering, characteristic of the plasma cut-off, does not appear due to peculiar features of wave propagation near the point of polarization degeneracy (where the X and O modes can not be treated as independent) [3]. In this case, perturbations of the averaged coupling efficiency due to the fluctuations inside the localized coupling region are usually negligible.
机译:普通(O)和非凡(X)电磁模式的线性变换在磁化等离子体中的等离子体截止附近是微波加热的先进方案的基础,并诊断磁性的磁化等离子体(其中中心密度超过截止值)融合研究。密度波动的显着影响是环形磁阱中的热磁化等离子体所固有的,在[1]中首先注意到线性变换过程中,其中考虑了这种现象的简单现象学模型。最近,通过一个更严格的分析,这张照片已大幅修改[2]。由于在存在密度波动的存在下求解线性相互作用区域中的截断的麦克斯韦方程,因此确定了低音耦合效率的显性效果是由于波束对沿着沿着波动波动的小角度散射向截止的传播路径,至少对对应于现代实验的参数范围的波动。在耦合区域之外,散射改变入射O波束,这影响其随后的变换和反射。这样,由于波传播附近的波传播的特征在于极化退化点附近的特征(其中x和o模式不能被视为独立的X和O模式,因此不出现等离子体切断的所谓增强散射,因此不会出现]。在这种情况下,由于局部耦合区域内的波动导致的平均耦合效率的扰动通常是可忽略不计的。

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