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Evolutions of zonal flows and turbulence in a tokamak edge plasma during electron cyclotron resonance heating

机译:电子回旋加速器共振加热过程中托卡马克边缘等离子体中纬向流和湍流的演变

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摘要

Geodesic acoustic mode (GAM) and low-frequency zonal flow (LFZF) are both observed through Langmuir probe arrays during electron cyclotron resonance heating (ECRH) on the HL-2A tokamak edge. The radial distributions of the amplitude and peak frequency of GAM in floating potential fluctuations are investigated through rake probe arrays under different ECRH powers. It is observed that the GAM frequency would decrease and the intensity of carbon line emission would increase as the ECRH power exceeds a certain threshold. The analyses suggest that the impurity ions may play an important role in the GAM frequency at the edge region. It is also found that during the ECRH phase besides the mean flow, both GAM and LFZF are strengthened. The total fluctuation power and the fraction of that power associated with zonal flows both increase with the ECRH power, consistent with a predator-prey model. The auto- and cross-bicoherence analyses show the coupling between GAM and its second harmonic during the ECRH phase. Moreover, the results also suggest that the couplings between GAM and the components with multiple GAM frequency are strengthened. These couplings may be important for GAM saturation during the ECRH phase.
机译:在HL-2A托卡马克边缘的电子回旋加速器共振加热(ECRH)期间,通过Langmuir探头阵列都观察到了测地声模(GAM)和低频纬向流(LFZF)。通过在不同ECRH功率下的耙探头阵列研究了GAM在浮动电势波动中幅度和峰值频率的径向分布。观察到,随着ECRH功率超过某个阈值,GAM频率将降低,碳线排放强度将增加。分析表明,杂质离子可能在边缘区域的GAM频率中起重要作用。还发现在ECRH阶段,除了平均流量外,GAM和LFZF都得到了增强。与食肉动物-猎物模型一致,总波动功率和与纬向流量相关的功率分数均随ECRH功率而增加。自相干和交叉双相干分析表明,在ECRH阶段,GAM及其二次谐波之间存在耦合。此外,结果还表明,GAM与具有多个GAM频率的组件之间的耦合得到加强。这些耦合对于ECRH阶段的GAM饱和可能很重要。

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  • 来源
    《Nuclear fusion》 |2013年第12期|123006.1-123006.11|共11页
  • 作者单位

    CAS Key Laboratory of Geospace Environment, Department of Modern Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China;

    CAS Key Laboratory of Geospace Environment, Department of Modern Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China;

    CAS Key Laboratory of Geospace Environment, Department of Modern Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China;

    Southwestern Institute of Physics, PO Box 432, Chengdu, Sichuan 610041, People's Republic of China;

    Southwestern Institute of Physics, PO Box 432, Chengdu, Sichuan 610041, People's Republic of China;

    Southwestern Institute of Physics, PO Box 432, Chengdu, Sichuan 610041, People's Republic of China;

    CAS Key Laboratory of Geospace Environment, Department of Modern Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China;

    CAS Key Laboratory of Geospace Environment, Department of Modern Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China;

    CAS Key Laboratory of Geospace Environment, Department of Modern Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China;

    CAS Key Laboratory of Geospace Environment, Department of Modern Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China;

    CAS Key Laboratory of Geospace Environment, Department of Modern Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China;

    CAS Key Laboratory of Geospace Environment, Department of Modern Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China;

    CAS Key Laboratory of Geospace Environment, Department of Modern Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China,Department of Physics and Astronomy, University of California at Los Angeles, Los Angeles, CA 90095, USA;

    CAS Key Laboratory of Geospace Environment, Department of Modern Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China;

    Southwestern Institute of Physics, PO Box 432, Chengdu, Sichuan 610041, People's Republic of China;

    Southwestern Institute of Physics, PO Box 432, Chengdu, Sichuan 610041, People's Republic of China;

    Southwestern Institute of Physics, PO Box 432, Chengdu, Sichuan 610041, People's Republic of China;

    Southwestern Institute of Physics, PO Box 432, Chengdu, Sichuan 610041, People's Republic of China;

    Southwestern Institute of Physics, PO Box 432, Chengdu, Sichuan 610041, People's Republic of China;

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