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Electron Bernstein wave heating via the slow X-B mode conversion process with direct launching from the high field side in LHD

机译:通过慢X-B模式转换过程对电子伯恩斯坦波进行加热,并从LHD的高场侧直接发射

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摘要

In the large helical device (LHD), direct oblique launching of the extraordinary (X-) mode from the high magnetic field side is available without installation of any additional mirror or installation of a launcher in the inner side of the torus. The launched X-mode first encounters the electron cyclotron resonance (ECR) layer from the high magnetic field side and then approaches the upper hybrid resonance (UHR) layer where mode conversion from the X-mode to electron Bernstein wave (EBW) occurs. Complete power absorption with a finite parallel component of the refractive index is promising whether the launched wave power is absorbed as the electromagnetic X-mode or is absorbed as electrostatic EBW even in the peripheral region. In the experiment, strong power absorption has been observed by direct oblique launching of the X-mode. Observation of the parametric decay wave suggests a fraction of the launched power reached the UHR layer that is located near the plasma boundary. The result of numerical analysis with three dimensional ray-tracing calculation using the dispersion equation in hot plasmas suggests that the launched X-mode is refracted toward the magnetic axis and strongly absorbed very close to the ECR layer that is located around ρ~0.5. The main part of the launched power is absorbed as the X-mode in the ECR layer where the electron temperature is sufficient high, while a fraction of the power reaches the UHR that is located in almost the plasma boundary.
机译:在大型螺旋装置(LHD)中,可以从高磁场侧直接倾斜发射非凡(X-)模式,而无需在圆环的内侧安装任何其他反射镜或安装发射器。发射的X模式首先从强磁场侧遇到电子回旋共振(ECR)层,然后到达上混合共振(UHR)层,在该层发生从X模式向电子伯恩斯坦波(EBW)的模式转换。完全有限的折射率平行分量的功率吸收是有希望的,即使在外围区域,发射的波功率是作为电磁X模吸收还是作为静电EBW吸收。在实验中,通过直接倾斜发射X模式观察到了强大的功率吸收。对参数衰减波的观察表明,发射功率的一部分到达了位于等离子体边界附近的UHR层。在热等离子体中使用色散方程进行三维射线追踪计算的数值分析结果表明,发射的X模向磁轴方向折射,并且非常强吸收,非常靠近ρ〜0.5附近的ECR层。发射功率的主要部分在电子温度足够高的ECR层中被吸收为X模式,而一部分功率到达几乎位于等离子体边界的UHR。

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