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首页> 外文期刊>Nuclear fusion >Core-localized Alfvenic modes driven by energetic ions in HL-2A NBI plasmas with weak magnetic shears
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Core-localized Alfvenic modes driven by energetic ions in HL-2A NBI plasmas with weak magnetic shears

机译:高能离子在弱磁剪切作用下的HL-2A NBI等离子体中由高能离子驱动的核局部Alfvenic模式

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摘要

Recent experimental results that are associated with the core-localized (i.e. normalized radius ρ = r/a< 0.5) Alfvenic modes in HL-2A neutral beam injection (NBI) plasmas with weak magnetic shears are reported. In the different plasma parameter regions, the energetic ions produced by the NBI drive multiple Alfvenic instabilities, such as the toroidal Alfven eigenmode (TAE), beta-induced Alfven eigenmode, reversed shear Alfven eigenmode (RSAE) and fishbone and energetic particle mode (EPM). Here, we focus on the high-frequency RSAE (HFRSAE) and resonant kinetic ballooning mode (rKBM). A group of downward-sweeping frequency coherent modes (HFRSAEs) with 100 <f< 500kHz and n = 3-7 are often observed with an increase in the edge safety factor, q_a. Their measured frequency is more than that of the TAEs, and f_(min) ~f_(TAE). The analysis suggests that these modes localize inside the high-order Alfv6n eigenmode (AE) gap of the Alfvenic continuum, and their eigenfrequency and eigenfunction depend on the q_(min) and q-profile. When the core plasma density is more than n_(e0) > 3.0 × 10~(19) m~(-3) and the impurity or supersonic molecular beam enters the bulk plasma, the profiles of the plasma density/pressure peak, and the magnetic shear is weak or negative. In this case, a group of multi-harmonic coherent modes (rKBMs) with 30 <f< 150kHz and n = 2-9 are observed through multiple diagnostic techniques, and f_(*Pi)/2 <f_(MHD) =f_(lab) - nf_(vφ) <f_(*pi), where f_(*pi) = ω_(*pi)/2π is the diamagnetic drift frequency of the thermal ion. It is found that the HFRSAEs can transit into the rKBMs when the density profile suddenly peaks. Neutron monitoring outside the vacuum chamber demonstrates that the HFRSAE and rKBM both degrade the confinement of the energetic ions. The rKBM instabilities also affect the bulk plasma performance.
机译:据报道,最近的实验结果与弱磁切变的HL-2A中性束注入(NBI)等离子体中的铁心局部化(即归一化半径ρ= r / a <0.5)的Alvvenic模式有关。在不同的等离子体参数区域中,由NBI产生的高能离子驱动多种Alfvenic不稳定性,例如环形Alfven本征模(TAE),β诱导的Alfven本征模,反向剪切Alfven本征模(RSAE)以及鱼骨和高能粒子模(EPM) )。在这里,我们专注于高频RSAE(HFRSAE)和共振动力学膨胀模式(rKBM)。随着边缘安全系数q_a的增加,经常观察到一组100 <f <500kHz且频率n = 3-7的向下扫描频率相干模式(HFRSAE)。它们的测量频率大于TAE,f_(min)〜f_(TAE)。分析表明,这些模式位于Alfvenic连续体的高阶Alfv6n本征模式(AE)间隙内,其本征频率和本征函数取决于q_(min)和q轮廓。当核心等离子体密度大于n_(e0)> 3.0×10〜(19)m〜(-3)且杂质或超音速分子束进入整体等离子体时,等离子体密度/压力峰的分布以及磁剪弱或为负。在这种情况下,通过多种诊断技术观察到一组30 <f <150kHz且n = 2-9的多谐波相干模(rKBMs),并且f _(* Pi)/ 2 <f_(MHD)= f_( lab)-nf_(vφ)<f _(* pi),其中f _(* pi)=ω_(* pi)/2π是热离子的反磁漂移频率。发现当密度分布突然达到峰值时,HFRSAE可以转变为rKBM。真空室外部的中子监测表明,HFRSAE和rKBM都降低了高能离子的约束。 rKBM的不稳定性也会影响整体等离子体的性能。

著录项

  • 来源
    《Nuclear fusion》 |2016年第3期|036018.1-036018.8|共8页
  • 作者单位

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

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

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

    Institute for Fusion Theory and Simulation, Zhejiang University, Hangzhou 310027, People's Republic of China;

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    Alfven eigenmode; resonant KBM; EPM; GFLDR;

    机译:Alfven本征模式共振KBM EPM;GFLDR;

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