J-PARC射频离子源提取光束的高速发射度测量

T. Shibata, K. Shinto, M. Wada, H. Oguri, K. Ikegami, K. Ohkoshi, K. Nanmo
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引用次数: 2

摘要

利用安装在RFQ入口的双缝发射度监测仪,测量了J-PARC 2MHz射频离子源的负离子(H -)束的发射度和Twiss参数的振荡。发射度监测仪配备了新开发的60 MS/s数据采集系统,可以在足够的时间分辨率下观测到几MHz的波束电流振荡。测量结果表明,束流相空间由:(1)束流芯中有直流分量;(2)在发散光晕中发生的2mhz振荡分量;(3)在波束晕中隐约存在双倍射频频率(4mhz)振荡。主分量为2mhz分量,从而决定波束发射度振荡频率。在本实验中,波束发射度的典型值为0.33 π mm-mrad,而2 MHz振荡幅度约为0.04 π mm-mrad。结果表明,占据射频源光束10%左右的高频振荡分量通过磁透镜聚焦系统传播了几米。
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High-speed emittance measurements for beams extracted from J-PARC RF ion source
Oscillation of emittance and Twiss parameters in the negative ion (H−) beam from the J-PARC 2MHz RF ion source is measured by application of a double-slit emittance monitor located at the RFQ entrance. The emittance monitor is equipped with a newly-developed 60 MS/s data acquisition system, so that beam current oscillations at a few MHz can be observed with enough time resolution. From the measurement, it is shown that the beam phase space consists of: (1) a Direct Current component in the beam core; (2) a 2 MHz oscillating component which takes place in the diverging halo; (3) a doubled RF frequency (4 MHz) oscillation which faintly exists in the beam halo. The major component is the 2 MHz component, which resultantly decides the beam emittance oscillation frequency. A typical value of the beam emittance in the present experiment is 0.33 π mm-mrad, while the amplitude of the 2 MHz oscillation is around 0.04 π mm-mrad. The results indicate that the high-frequency oscillation component occupying about ten-percent of the beam from the RF source travels a few meters passing through a magnetic lens focusing system.
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