An overview of the energetic electron induced instabilities with high-power ECRH on HL-2A

In this paper, an overview of the magnetohydrodynamic instabilities induced by energetic electrons on HL-2A is given and some new phenomena with high-power electron cyclotron resonance heating (ECRH) are presented. A toroidal Alfven eigenmode with frequency from 200 to 350 kHz is identified during powerful ECRH. In the lower frequency range from 10 to 35 kHz, which is in the beta-induced Alfven eigenmode frequency range, the coexistence of multi-mode is found during the high-power ECRH for the first time. The spectra become wide when the power is sufficiently high. The frequencies of the modes increase with and are much lower than the Alfven frequency. The relationship between the mode frequency and (7/4 + Te/Ti)1/2 (Ti)1/2 can be obtained by statistical data analysis. Between the two previous frequency ranges, a group of new modes with frequencies from 50 to 180 kHz is observed with high-power ECRH and neutral beam injection heating together. The modes have clear frequency chirping within several milliseconds or several tens of milliseconds, which are identified as energetic particle mode like instabilities. The new features of the fishbone instability excited by energetic electrons are identified. It is interesting to find the frequency jump phenomena in the high-power ECRH. The difference between the low and high frequencies increases with ECRH power. The frequency jumps between 8 and 15 kHz within about 25 ms periodically, when the power is 1.2 MW.

[1]  F. Zonca,et al.  Fishbone instability excited by circulating electrons , 2007 .

[2]  A. Tuccillo,et al.  Lower hybrid wave produced supra-thermal electrons and fishbone-like instability in FTU , 2009 .

[3]  Liu Chen Alfvén waves: a journey between space and fusion plasmas , 2008 .

[4]  Turnbull,et al.  Observation of beta-induced Alfvén eigenmodes in the DIII-D tokamak. , 1993, Physical review letters.

[5]  H. Furth Unstable Precession under the Influence of Drag Forces , 1965 .

[6]  J. Lister,et al.  Alfven eigenmode experiments in tokamaks and stellarators , 1997 .

[7]  K. Wong,et al.  A review of Alfvén eigenmode observations in toroidal plasmas , 1999 .

[8]  A. Shimizu,et al.  Energetic-particle modes driven by suprathermal electrons produced by off-axis second harmonic ECRH in compact helical system (CHS) , 2010 .

[9]  Yi Liu,et al.  Destabilization of the internal kink mode by energetic electrons on the HL-2A tokamak , 2009 .

[10]  M. Valovic,et al.  Quasi-stationary high β plasmas and fast particle instabilities in the COMPASS-D tokamak with ECRH and LHCD , 2000 .

[11]  Harvey,et al.  Internal kink instability during off-axis electron cyclotron current drive in the DIII-D tokamak , 1999, Physical review letters.

[12]  Redistribution of suprathermal electrons due to fishbone frequency jumps. , 2009, Physical review letters.

[13]  Masayasu Sato,et al.  Investigation of high-n TAE modes excited by minority-ion cyclotron heating in JT-60U , 1995 .

[14]  W. Lotz,et al.  INVESTIGATION OF PLASMA CONFINEMENT IN A TOROIDAL THETA-PINCH WITH M + S- LIKE CONFIGURATIONS , 1963 .

[15]  J. Snipes,et al.  Fast electron driven Alfvén eigenmodes in the current rise in Alcator C-MOD , 2008 .

[16]  Y. Liu,et al.  Observation of internal kink instability purely driven by suprathermal electrons in the HL-1M tokamak , 2002 .

[17]  Investigation of fast particle driven modes on Alcator C-Mod , 2000 .

[18]  J. Byun,et al.  Atmospheric-pressure plasma sources for biomedical applications , 2012 .

[19]  D. Brower,et al.  Energetic-electron-driven instability in the helically symmetric experiment. , 2009, Physical review letters.

[20]  F. Imbeaux,et al.  Temperature oscillating regimes in Tore Supra diagnosed by MHD activity , 2006 .

[21]  G. Yuan,et al.  Features of ion and electron fishbone instabilities on HL-2A , 2010 .

[22]  Chengdu,et al.  Electron fishbones: theory and experimental evidence , 2007, 0707.2852.

[23]  L. Chen,et al.  Theory and simulation of discrete kinetic beta induced Alfvén eigenmode in tokamak plasmas , 2010 .

[24]  Y. Liu,et al.  Overview of HL-2A experiment results , 2007 .

[25]  M. Rosenbluth,et al.  Chapter 5: Physics of energetic ions , 1999 .

[26]  S. Jardin,et al.  Dynamic modeling of transport and positional control of tokamaks , 1986 .

[27]  L. Chen,et al.  Theory of Alfvén waves and energetic particle physics in burning plasmas , 2007 .