J-PARC的110 mA操作使rf驱动的氢离子源停止

A. Ueno, K. Ohkoshi, K. Ikegami, A. Takagi, K. Shinto, H. Oguri
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引用次数: 3

摘要

日本质子加速器研究中心(J-PARC)停止了rf驱动的氢离子源(IS),已经稳定运行了大约6年。自2018年9月以来,J-PARC 400 MeV直线加速器在从is注入60 mA束流时,以50 mA的设计H -离子束强度(IH -)稳定运行。在每个约3个月的J-PARC运行结束时,IS提供52.5 keV 72毫安的光束,用于LINAC 60毫安的加速度。在试验台上预测的IS优越的发射效率被证明是高RFQ加速效率94.3% (IH−= 67.9 mA)。采用了几种独特的措施,如在氢等离子体中加入少量的水分子,产生了适合RFQ的横向发射的高强度光束;低温(约70℃)操作45°锥形16毫米厚等离子体电极与精确的铯密度控制;氢等离子体中的杂质消除及过滤场优化用50瓦30 mhz射频驱动的连续波等离子体点火器,等等。本文介绍了该系统在试验台110毫安时的运行结果。一个65 keV 110 mA的氢离子束,其中约103 mA位于用于普通RFQ设计的横向发射内,在占空因数为4.5% (1 ms x 45 Hz)的情况下稳定运行。在所需束流能量(WH-)上没有任何发射度变化的IH -的有趣关系推导为IH - (WH-) = 71.2 x (WH- / 52.5)^2.03。IS是下一代高能H−LINACs的基准器件,目标是达到100ma级强度。
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110 mA operation of J-PARC cesiated RF-driven H− ion source
The Japan Proton Accelerator Research Complex (J-PARC) cesiated RF-driven H− ion source (IS) has been stably operated for about six years. From Sep. 2018, the J-PARC 400 MeV LINAC has been steadily operated with the design H− ion beam intensity (IH−) of 50 mA, when a 60 mA beam is injected from the IS. At each end of about 3 months J-PARC operation, the IS supplies a 52.5 keV 72 mA beam for the LINAC 60 mA acceleration. The IS superior emittances predicted in a test-stand were proven by the high RFQ acceleration efficiency of 94.3 % (IH− = 67.9 mA). The high intensity beam with transverse emittances suitable for the RFQ is produced with several unique measures, such as slight water molecule addition into hydrogen plasma; low temperature (about 70 °C) operation of 45°-tapered 16-mm thick plasma electrode with the precise cesium density control; impurity elimination in the hydrogen plasma along with the filter-field optimization; continuous-wave igniter plasma driven with a 50-W 30-MHz RF, and so on. The 110 mA operation results of the IS in the test-stand are presented in this paper. A 65 keV 110 mA H− ion beam, about 103 mA of which was inside the transverse emittances used for a common RFQ design, was stably operated with a duty factor of 4.5 % (1 ms x 45 Hz). The interesting relationship of the IH− without any emittance blowups upon the required beam energy (WH-) was derived as IH−(WH−) = 71.2 x (WH- / 52.5)^2.03. The IS is the benchmark one for the next generation high energy H− LINACs aiming for 100 mA class intensity.
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