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Takashi MINAMI, Shohei ARAI, Naoki KENMOCH, Hiroaki YASHIRO, Chihiro TAKAHASHI, Shinji KOBAYASHI, Tohru MIZUUCHI, Shinsuke OHSHIMA, Satoshi YAMAMOTO, Hiroyuki OKADA, Kazunobu NAGASAKI, et al. Present Status of the Nd:YAG Thomson Scattering System Development for Time Evolution Measurement of Plasma Profile on Heliotron J[J]. Plasma Science and Technology, 2013, 15(3): 240-243. DOI: 10.1088/1009-0630/15/3/10
Citation: Takashi MINAMI, Shohei ARAI, Naoki KENMOCH, Hiroaki YASHIRO, Chihiro TAKAHASHI, Shinji KOBAYASHI, Tohru MIZUUCHI, Shinsuke OHSHIMA, Satoshi YAMAMOTO, Hiroyuki OKADA, Kazunobu NAGASAKI, et al. Present Status of the Nd:YAG Thomson Scattering System Development for Time Evolution Measurement of Plasma Profile on Heliotron J[J]. Plasma Science and Technology, 2013, 15(3): 240-243. DOI: 10.1088/1009-0630/15/3/10

Present Status of the Nd:YAG Thomson Scattering System Development for Time Evolution Measurement of Plasma Profile on Heliotron J

Funds: supported by the Collaboration Program of the Laboratory for Complex Energy Processes, IAE, Kyoto University and the NIFS Collaborative Research Program (NIFS10KUHL030, NIFS09KUHL028, NIFS10KUHL033)
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  • Received Date: January 18, 2012
  • A new high repetition rate Nd:YAG Thomson scattering system is developed for the Heliotron J helical device. A main purpose of installing the new system is the temporal evolution measurement of a plasma profile for improved confinement physics such as the edge transport barrier (H-mode) or the internal transport barrier of the helical plasma. The system has 25 spatial points with ~10 mm resolution. Two high repetition Nd:YAG lasers (> 550 mJ@ 50 Hz) realize the measurement of the time evolution of the plasma profile with ~10 ms time intervals. Scattered light is collected by a large concave mirror (D=800 mm, f/2.25) with a solid angle of ~100 mstr and transferred to interference filter polychromators by optical fiber bundles in a staircase form. The signal is amplified by newly designed fast preamplifiers with DC and AC output, which reduces the low frequency background noise. The signals are digitized with a multi-event QDC, fast gated integrators. The data acquisition is performed by a VME-based system operated by the CINOS.
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