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Yaoyu XIE (谢耀禹), Kaijun ZHAO (赵开君), Zhipeng CHEN (陈志鹏), Jiaqi DONG (董家齐), Kimitaka ITOH, Zhongyong CHEN (陈忠勇), Yuejiang SHI (石跃江), Yonghua DING (丁永华), Jun CHENG (程钧), Longwen YAN (严龙文), Hai LIU (刘海), Zhifeng CHENG (程芝峰), Zhoujun YANG (杨州军), Nengchao WANG (王能超), Lu WANG (王璐), Jianqiang XU (许健强), Yunfeng LIANG (梁云峰), J-TEXT Team. Toroidal component of velocity for geodesic acoustic modes in the edge plasmas of the J-TEXT tokamak[J]. Plasma Science and Technology, 2021, 23(10): 105102. DOI: 10.1088/2058-6272/ac0ccd
Citation: Yaoyu XIE (谢耀禹), Kaijun ZHAO (赵开君), Zhipeng CHEN (陈志鹏), Jiaqi DONG (董家齐), Kimitaka ITOH, Zhongyong CHEN (陈忠勇), Yuejiang SHI (石跃江), Yonghua DING (丁永华), Jun CHENG (程钧), Longwen YAN (严龙文), Hai LIU (刘海), Zhifeng CHENG (程芝峰), Zhoujun YANG (杨州军), Nengchao WANG (王能超), Lu WANG (王璐), Jianqiang XU (许健强), Yunfeng LIANG (梁云峰), J-TEXT Team. Toroidal component of velocity for geodesic acoustic modes in the edge plasmas of the J-TEXT tokamak[J]. Plasma Science and Technology, 2021, 23(10): 105102. DOI: 10.1088/2058-6272/ac0ccd
  • The toroidal component of the velocity for geodesic acoustic modes (GAMs) is first demonstrated. Multiple Langmuir probe arrays set up near the top tokamak of the J-TEXT were utilized for this study. A significant peak at the GAM frequency is observed in Mach number fluctuations. The toroidal velocity for the GAMs is estimated as ∼10–100 m s−1 and increases with the poloidal velocity. The ratio of toroidal component to the poloidal one of the velocity is mainly located in the interval between 0.3 and 1.0. With higher safety factors q, the ratio almost does not change with decreasing the safety factor, whereas it goes up sharply at low q. The coherencies between poloidal electric fields and Mach number fluctuations in turbulence frequency bands are also evaluated, and are higher than those between radial electric fields and Mach number fluctuations.
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