Experimental and simulation analysis of Weakly Coherent Modes in I-mode discharges on EAST

Y.J. Liu; Z.X. Liu; T.Y. Xia; T. Zhang; A.D. Liu; J. Liu; C.C. Deng; K.X. Ye; K.N. Geng; G.S. Li; F.F. Long; J.Y. Li; P.C. Li; K.N. Yang; Q. Zang; A. Ti; H.L. Zhao; H.Q. Liu; H. Li; J.L. Xie; T. Lan; W.Z. Mao; C. Zhou; W.X. Ding; G. Zhuang; W.D. Liu; G.Q. Li; X. Gao

doi:10.1088/1741-4326/ad4b3f

Nuclear Fusion (Jan 2024)

Experimental and simulation analysis of Weakly Coherent Modes in I-mode discharges on EAST

Y.J. Liu,
Z.X. Liu,
T.Y. Xia,
T. Zhang,
A.D. Liu,
J. Liu,
C.C. Deng,
K.X. Ye,
K.N. Geng,
G.S. Li,
F.F. Long,
J.Y. Li,
P.C. Li,
K.N. Yang,
Q. Zang,
A. Ti,
H.L. Zhao,
H.Q. Liu,
H. Li,
J.L. Xie,
T. Lan,
W.Z. Mao,
C. Zhou,
W.X. Ding,
G. Zhuang,
W.D. Liu,
G.Q. Li,
X. Gao

Affiliations

Y.J. Liu: ORCiD; Institute of Plasma Physics, Chinese Academy of Sciences , Hefei 230031, China
Z.X. Liu: School of Nuclear Science and Technology, University of Science and Technology of China , Anhui, Hefei 230026, China
T.Y. Xia: Institute of Plasma Physics, Chinese Academy of Sciences , Hefei 230031, China
T. Zhang: ORCiD; Institute of Plasma Physics, Chinese Academy of Sciences , Hefei 230031, China
A.D. Liu: ORCiD; School of Nuclear Science and Technology, University of Science and Technology of China , Anhui, Hefei 230026, China
J. Liu: ORCiD; School of Nuclear Science and Technology, University of Science and Technology of China , Anhui, Hefei 230026, China
C.C. Deng: School of Nuclear Science and Technology, University of Science and Technology of China , Anhui, Hefei 230026, China
K.X. Ye: ORCiD; Institute of Plasma Physics, Chinese Academy of Sciences , Hefei 230031, China
K.N. Geng: ORCiD; Institute of Plasma Physics, Chinese Academy of Sciences , Hefei 230031, China
G.S. Li: Institute of Plasma Physics, Chinese Academy of Sciences , Hefei 230031, China
F.F. Long: ORCiD; School of Nuclear Science and Technology, University of Science and Technology of China , Anhui, Hefei 230026, China
J.Y. Li: School of Nuclear Science and Technology, University of Science and Technology of China , Anhui, Hefei 230026, China
P.C. Li: ORCiD; School of Nuclear Science and Technology, University of Science and Technology of China , Anhui, Hefei 230026, China
K.N. Yang: ORCiD; School of Nuclear Science and Technology, University of Science and Technology of China , Anhui, Hefei 230026, China
Q. Zang: Institute of Plasma Physics, Chinese Academy of Sciences , Hefei 230031, China
A. Ti: Institute of Plasma Physics, Chinese Academy of Sciences , Hefei 230031, China
H.L. Zhao: Institute of Plasma Physics, Chinese Academy of Sciences , Hefei 230031, China
H.Q. Liu: ORCiD; Institute of Plasma Physics, Chinese Academy of Sciences , Hefei 230031, China
H. Li: School of Nuclear Science and Technology, University of Science and Technology of China , Anhui, Hefei 230026, China
J.L. Xie: School of Nuclear Science and Technology, University of Science and Technology of China , Anhui, Hefei 230026, China
T. Lan: ORCiD; School of Nuclear Science and Technology, University of Science and Technology of China , Anhui, Hefei 230026, China
W.Z. Mao: ORCiD; School of Nuclear Science and Technology, University of Science and Technology of China , Anhui, Hefei 230026, China
C. Zhou: School of Nuclear Science and Technology, University of Science and Technology of China , Anhui, Hefei 230026, China
W.X. Ding: School of Nuclear Science and Technology, University of Science and Technology of China , Anhui, Hefei 230026, China
G. Zhuang: School of Nuclear Science and Technology, University of Science and Technology of China , Anhui, Hefei 230026, China
W.D. Liu: School of Nuclear Science and Technology, University of Science and Technology of China , Anhui, Hefei 230026, China
G.Q. Li: Institute of Plasma Physics, Chinese Academy of Sciences , Hefei 230031, China
X. Gao: ORCiD; Institute of Plasma Physics, Chinese Academy of Sciences , Hefei 230031, China

DOI: https://doi.org/10.1088/1741-4326/ad4b3f
Journal volume & issue: Vol. 64, no. 7
p. 076045

Abstract

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This paper reports the recent observation of a weakly coherent mode (WCM) within a conventional reflectometer on EAST and successfully determines its poloidal wavenumber range. During the transition from the L-mode to I-mode, the line-averaged density remains nearly unchanged while a significant change is observed in the electron cyclotron emission (ECE) signals at the boundary. The difference between the signals for the two channels at the edge increased, coinciding with the appearance of the WCM and a simultaneous rise in the boundary electron temperature. Further investigation unveiled the modulating role of edge temperature ring oscillation (ETRO) (Liu et al 2020 Nucl. Fusion 60 126016) on high-frequency density fluctuations. Statistical results unveil an inverse relationship between the centeral frequency of the WCM and q _95 . Simulation results provide additional insights, demonstrating that the simulated ‘WCM’ in the density fluctuations aligns with experimental data in terms of center frequency. Additionally, the radial distribution of the simulated ‘WCM’ closely corresponds to regions with the strongest electron temperature gradients. Finally, through a cross-correlation analysis of the simulated fluctuations, the following phase relationship for the wavenumber range of ‘WCM’ was observed: $\alpha_{\widetilde{T}_e} \gt \alpha_{\widetilde{n}_i}\sim\alpha_{\widetilde{\phi}} \gt \alpha_{\widetilde{T}_i}$ .

Published in Nuclear Fusion

ISSN: 0029-5515 (Print); 1741-4326 (Online)
Publisher: IOP Publishing
Country of publisher: United Kingdom
LCC subjects: Science: Physics: Nuclear and particle physics. Atomic energy. Radioactivity
Website: https://iopscience.iop.org/journal/0029-5515

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