Production of Hydrogen Plasma by Compact ECR Source for Efficient Volume Generation of H− Ions

P. Singh, D. Sahu, R. Narayanan, A. Ganguli, S. Kar, R. D. Tarey
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Abstract

Hydrogen plasma produced inside a compact ECR plasma source (CEPS)1 was allowed to expand into a large expansion chamber (dia. ≈ 50 cm, length ≈ 75 cm). Plasma parameters were measured using an on-axis Langmuir Probe. The CEPS uses NdFeB ring magnets with a complex field structure that has a magnetic mirror trap near the ECR zone followed by an on-axis magnetic null within the source region, and a monotonically decreasing field in the expansion chamber. Typically, at ≈ 600 W microwave power (2.45 GHz), 0.3–2 mTorr hydrogen pressure, the plasma density $n\approx 10^{10}\ \text{cm}^{-3}$ and electron temperature $T_{\mathrm{e}}\approx 25\ \ \text{eV}$ in the expansion chamber near the source, while further downstream $n$ and $T_{\mathrm{e}}$ are reduced to ≈ 109 cm−3 and 5 eV, respectively2. However, for 3–10 mTorr the plasma contains two electron populations - a high density, cold, bulk population and a low-density, warm population ($n_{w}/n\approx 0.01;\ T_{w}/T_{e}\approx 10$). Another feature observed at the higher pressures is that $T_{\mathrm{e}}$ cools to less than 1 eV about ≈ 30 cm from the source mouth. Such low $T_{\mathrm{e}}$ bulk electrons are important for generation of H− ions by the volume production mode, which may be preferred over the caesiated grid method due to maintenance issues associated with the latter3. An interesting feature of the plasma is that the normalized plasma density and magnetic field profiles overlap fairly accurately indicating very little cross-field transport of the hydrogen plasma. In general, one finds from the experiments that the nature of the CEPS magnetic field is such as to promote efficient electron heating and high $T_{\mathrm{e}}$, which are not desirable for volume production of H− ions. To achieve the latter, another field configuration that eliminates the adverse effects of the magnetic mirror and the null has been set up and results from the latter configuration will be presented at the conference.
用紧凑ECR源生产氢等离子体以高效生成氢离子
在紧凑的ECR等离子体源(CEPS)内产生的氢等离子体被允许扩展到一个大的膨胀室(直径。≈50 cm,长度≈75 cm)。等离子体参数测量使用轴上朗缪尔探针。cceps使用具有复杂场结构的钕铁硼环形磁体,在ECR区附近有一个磁镜陷阱,然后在源区域内有一个轴向磁零,在膨胀室中有一个单调递减的场。通常,在约600 W微波功率(2.45 GHz), 0.3-2 mTorr氢压下,源附近膨胀腔内的等离子体密度$n\约10^{10}\ \text{cm}^{-3}$和电子温度$T_ \ mathm {e}}$约25\ \ mathm {eV}$,而下游的$n$和$T_ \ mathm {e}}$分别降至≈109 cm−3和5 eV 2。然而,在3-10 mTorr时,等离子体包含两个电子居群——高密度、冷、大块居群和低密度、热居群($n_{w}/n\约0.01;$ T_{w}/T_{e}\约10$)。在较高压力下观察到的另一个特征是$T_{\ mathm {e}}$在离源口约≈30 cm处冷却到小于1 eV。这种低$T_{\ mathm {e}}$的体电子对于通过批量生产模式产生H -离子是重要的,由于与后者相关的维护问题,它可能比铯网格方法更优选。等离子体的一个有趣特征是,归一化等离子体密度和磁场剖面相当精确地重叠,表明氢等离子体的跨场输运很少。总的来说,从实验中发现,CEPS磁场的性质是促进有效的电子加热和高$T_{\ mathm {e}}$,这对于H -离子的批量生产是不理想的。为了实现后者,已经建立了另一种消除磁镜和null不利影响的场配置,后者配置的结果将在会议上展示。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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