螺旋核的形成:导致径向输运屏障和自发轴向等离子体分离的全球输运分岔

S. C. Thakur
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引用次数: 0

摘要

我们报道了射频器件中螺旋核的形成伴随着径向输运屏障的形成和同时的轴向等离子体分离;通过由输运分岔引起的自组织全局过渡[1]。来自Langmuir探测器和快速成像的证据表明,传输屏障的径向范围与螺旋核的宽度相似。利用光谱学和中性压力测量,我们同时观察到轴向等离子体分离,它遵循与径向输运分岔相关的相同的滞后模式。我们报告了在这一转变过程中平均和波动曲线的巨大变化。这种自发的自组织全局跃迁是普遍的,但跃迁阈值取决于螺旋源参数。二维分岔图阐明了射频等离子体源的各种运行机制(电容耦合等离子体、电感耦合等离子体、螺旋分离、螺旋连接),允许在同一设备中研究基本的等离子体不稳定性、湍流和输运,以及与导流器相关的等离子体分离。自发等离子体脱离对设计用于研究等离子体材料相互作用(PMI)的类似射频设备的相关性具有严重影响[2],[3]。此外,这也使我们有机会研究与分离等离子体相关的不稳定性、湍流和输运[4],[5]。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Helicon Core Formation: A Global Transport Bifurcation Leading to a Radial Transport Barrier and Spontaneous Axial Plasma Detachment
We report that helicon core formation in rf devices is accompanied by the formation of a radial transport barrier and simultaneous axial plasma detachment; via a self-organized global transition due to a transport bifurcation [1] . Evidence from both Langmuir probes and fast imaging show that the radial extent of the transport barrier is similar to the width of the helicon core. Using spectroscopy and neutral pressure measurements, we simultaneously observe axial plasma detachment, which follow the same hysteresis patterns associated with the radial transport bifurcation. We report dramatic changes in both mean and fluctuation profiles across this transition. This spontaneous self-organized global transition is universal, but the transition-threshold depends on the helicon source parameters. 2-D bifurcation diagrams elucidate various regimes of operation of rf plasma sources (Capacitively Coupled Plasmas, Inductively Coupled Plasmas, Helicon-detached, helicon-attached), allowing access to study basic plasma instabilities, turbulence and transport, as well as divertor-relevant plasma detachment in the same device. Spontaneous plasma detachment has serious implications on the relevance of similar rf devices [2] , [3] designed to study Plasma Material Interactions (PMI). In addition, this also gives us the opportunity to study instabilities, turbulence and transport associated with detached plasmas [4] , [5] .
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