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Hot electron plasmas trapped in helical magnetic surfaces

机译:捕获在螺旋磁性表面中的热电子等离子体

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摘要

Experimental studies on nonneutral (pure electron) plasmas of finite temperature, trapped in helical closed magnetic surfaces have been conducted. The helical electron plasmas are produced with thermal electrons launched from the outside of the last closed flux surface (LCFS). About 150 μs after the electron injection, the plasmas reach equilibrium state. Around the LCFS, a steep gradient of plasma space potential φ s is formed. The corresponding radial electric field is about 2.5 kV/m. On the other hand, around the magnetic axis of helical magnetic surfaces, φ s is almost constant, indicating that there are little electrons there. The volume-averaged electron density is on the order of 1013 m–3, smaller than the Brillouin density limit. The confinement time seems to be limited by a disruptive instability, and is so far about 1.5 ms.
机译:已经进行了有限温度的非中性(纯电子)等离子体的实验研究,该等离子体被困在螺旋形封闭的磁性表面中。螺旋电子等离子体是由从最后一个封闭通量表面(LCFS)的外部发射的热电子产生的。电子注入后约150μs,等离子体达到平衡状态。在LCFS周围,形成了等离子体空间电势φs 的陡峭梯度。相应的径向电场约为2.5 kV / m。另一方面,在螺旋磁性表面的磁轴周围,φs 几乎是恒定的,这表明那里几乎没有电子。体积平均电子密度约为1013 m–3 ,小于布里渊密度极限。限制时间似乎受到破坏性不稳定性的限制,到目前为止大约为1.5 ms。

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