-
- OKADA Hiroyuki
- Institute of Advanced Energy, Kyoto University, Gokasho, Uji 611-0011, Japan
-
- NOMURA Kota
- Graduate School of Energy Science, Kyoto University, Gokasho, Uji 611-0011, Japan
-
- WATADA Hiroto
- Graduate School of Energy Science, Kyoto University, Gokasho, Uji 611-0011, Japan
-
- KOBAYASHI Shinji
- Institute of Advanced Energy, Kyoto University, Gokasho, Uji 611-0011, Japan
-
- LEE Hyunyong
- Graduate School of Energy Science, Kyoto University, Gokasho, Uji 611-0011, Japan
-
- MIZUUCHI Tohru
- Institute of Advanced Energy, Kyoto University, Gokasho, Uji 611-0011, Japan
-
- NAGASAKI Kazunobu
- Institute of Advanced Energy, Kyoto University, Gokasho, Uji 611-0011, Japan
-
- MINAMI Takashi
- Institute of Advanced Energy, Kyoto University, Gokasho, Uji 611-0011, Japan
-
- YAMAMOTO Satoshi
- Institute of Advanced Energy, Kyoto University, Gokasho, Uji 611-0011, Japan
-
- OHSHIMA Shinsuke
- Kyoto University Pioneering Research Unit for Next Generation, Gokasho, Uji 611-0011, Japan
-
- TAKEUCHI Masaki
- Institute of Advanced Energy, Kyoto University, Gokasho, Uji 611-0011, Japan
-
- KONOSHIMA Shigeru
- Institute of Advanced Energy, Kyoto University, Gokasho, Uji 611-0011, Japan
-
- MUTOH Takashi
- National Institute for Fusion Science,322-6 Oroshi-cho, Toki 509-5292, Japan
-
- MUKAI Kiyofumi
- Graduate School of Energy Science, Kyoto University, Gokasho, Uji 611-0011, Japan
-
- YAMAMOTO Kento
- Graduate School of Energy Science, Kyoto University, Gokasho, Uji 611-0011, Japan
-
- SUWA Masashige
- Graduate School of Energy Science, Kyoto University, Gokasho, Uji 611-0011, Japan
-
- YASHIRO Hiroaki
- Graduate School of Energy Science, Kyoto University, Gokasho, Uji 611-0011, Japan
-
- YOSHINO Hayao
- Graduate School of Energy Science, Kyoto University, Gokasho, Uji 611-0011, Japan
-
- NAKAMURA Yuji
- Graduate School of Energy Science, Kyoto University, Gokasho, Uji 611-0011, Japan
-
- HANATANI Kiyoshi
- Institute of Advanced Energy, Kyoto University, Gokasho, Uji 611-0011, Japan
-
- SANO Fumimichi
- Institute of Advanced Energy, Kyoto University, Gokasho, Uji 611-0011, Japan
抄録
The effect of the magnetic configuration on fast-ion confinement is one of the most important topics for helical devices. Fast-ion velocity distributions have been investigated using ion cyclotron range of frequencies (ICRF) minority heating in Heliotron J with special emphasis on the effect of the toroidal ripple (bumpiness) of the magnetic field strength. In measurements of the fast-ion tail generated by ICRF minority heating, a high bumpiness configuration is found to be preferable for tail formation. However, the measurement area based on the line of sight of the fast-ion detector was restricted in this experiment. Due to the complexity of the magnetic field in Heliotron J, three-dimensional analysis is required to interpret the experimental results. Monte-Carlo simulations were performed. The calculation results agree well with the experimental results for high-energy tail formation. The effective temperature of minority protons was estimated.
収録刊行物
-
- Plasma and Fusion Research
-
Plasma and Fusion Research 6 2402063-2402063, 2011
一般社団法人 プラズマ・核融合学会
- Tweet
詳細情報 詳細情報について
-
- CRID
- 1390282680230053120
-
- NII論文ID
- 130002059533
-
- ISSN
- 18806821
-
- 本文言語コード
- en
-
- データソース種別
-
- JaLC
- Crossref
- CiNii Articles
- KAKEN
-
- 抄録ライセンスフラグ
- 使用不可