Observation of GAM Induced by Energetic Electrons and NL Interactions among GAM, BAEs and Tearing Modes on the HL-2A Tokamak
Creators
- 1. Southwestern Institute of Physics, Chengdu (China)
- 2. National Institute for Fusion Science, Toki (Japan)
- 3. College of Physical Science and Technology, Sichuan University, Chengdu (China)
Description
Full text: The very low-frequency (LF) Alfvenic and acoustic fluctuations, such as beta-induced Alfven eigenmode (BAE), and geodesic acoustic mode (GAM), are presently of considerable interest in the present-day fusion and future burning plasmas. The low-frequency waves can significantly affect the plasma performance, and induce the particle losses and reduce the plasma self-heating. These LF instabilities can play a key role in turbulence and anomalous transport regulation, especially, while there is significant fraction of high energy particles in plasma. They can be used as energy channels to transfer the fusion-born-alpha-particle energy to the thermonuclear plasma, i.e., GAM/BAE channeling. The energetic-electron and magnetic-island induced BAEs had been observed and investigated on HL-2A in the previous works. In the present paper, we will present our further works about the LF Alfvenic and acoustic modes, and it is reported that the first experimental results are associated with the GAM induced by energetic-electrons (termed eEGAM) in HL-2A Ohmic plasma. The energetic-electrons are generated by parallel electric fields during magnetic reconnection associated with tearing mode (TM). The energy spectra, which detected by Cadmium-telluride (CdTe) scintillators, indicate that the energetic electrons redistribute during strong TM. The magnetic fluctuation spectrogram indicates that the eEGAM is always accompanied by TM and BAEs. The eEGAM is not observed in the absence of strong TM and BAEs, and its mode frequency always complies with f GAM = f BAE2 - f TM , f GAM = f BAE1 + f TM as well as f GAM = (f BAE1 + fBAE2) / 2. The eEGAM localizes in the core plasma, i.e., in the vicinity of q = 2 surface where the ion Landau damping γi is larger than the edge due to γi α exp(-q2), and is very different from that excited by the drift-wave turbulence in the edge plasma. The analysis indicated that the eEGAM is provided with the magnetic components, whose intensities depend on the poloidal angles, and its mode numbers are |m/n| = 2/0 which are consistent with the theoretical prediction. The new findings give a deep insight into the underlying physics mechanism for the excitation of the LF Alfvenic/acoustic fluctuation and zonal flows (ZFs). (author)
Additional details
Publishing Information
- Imprint Title
- 24. IAEA Fusion Energy Conference. Programme and Book of Abstracts
- Imprint Pagination
- 789 p.
- Journal Page Range
- p. 54
- Report number
- IAEA-CN--197
Conference
- Title
- 24. IAEA Fusion Energy Conference
- Acronym
- FEC 2012
- Dates
- 8-13 Oct 2012
- Place
- San Diego, CA (United States)
INIS
- Country of Publication
- International Atomic Energy Agency (IAEA)
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 44060355
- Subject category
- S70: PLASMA PHYSICS AND FUSION TECHNOLOGY;
- Resource subtype / Literary indicator
- Conference
- Descriptors DEI
- ALFVEN WAVES; ALPHA PARTICLES; CADMIUM TELLURIDES; ELECTRIC FIELDS; ENERGY SPECTRA; EXCITATION; FLUCTUATIONS; HL-2A TOKAMAK; INTERACTIONS; LANDAU DAMPING; MAGNETIC ISLANDS; MAGNETIC RECONNECTION; PHOSPHORS; PLASMA; SOLID SCINTILLATION DETECTORS; SURFACES; TAIL ELECTRONS; TEARING INSTABILITY; TRANSPORT REGULATIONS; WAVE PROPAGATION
- Descriptors DEC
- CADMIUM COMPOUNDS; CHALCOGENIDES; CHARGED PARTICLES; CLOSED PLASMA DEVICES; DAMPING; ELECTRONS; ELEMENTARY PARTICLES; ENERGY-LEVEL TRANSITIONS; FERMIONS; HYDROMAGNETIC WAVES; INSTABILITY; IONIZING RADIATIONS; LAWS; LEPTONS; MAGNETIC FIELD CONFIGURATIONS; MEASURING INSTRUMENTS; PLASMA INSTABILITY; PLASMA MACROINSTABILITIES; RADIATION DETECTORS; RADIATIONS; REGULATIONS; SCINTILLATION COUNTERS; SPECTRA; TELLURIDES; TELLURIUM COMPOUNDS; THERMONUCLEAR DEVICES; TOKAMAK DEVICES; VARIATIONS
Optional Information
- Secondary number(s)
- EX/5--3