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首页> 外文期刊>Research report NIFS series >Alfven Eigenmodes and Geodesic Acoustic Modes Driven by Energetic Ions in an LHD Plasma with Non-monotonic Rotational Transform Profile
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Alfven Eigenmodes and Geodesic Acoustic Modes Driven by Energetic Ions in an LHD Plasma with Non-monotonic Rotational Transform Profile

机译:具有非单调旋转变换轮廓的LHD等离子体中高能离子驱动的Alfven本征模和测地声模

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In the Large Helical Device (LHD), a reversed magnetic shear (RS) configuration having non-monotonic rotational transform profile was formed by intense counter neutral beam (NB) current drive. In the RS configuration helical plasma, the reversed shear Alfven eigenmode (RSAE) with n=1 toroidal mode number was identified together with energetic-ion-driven geodesic acoustic mode (GAM) with n=0. Temporal sweeping of the RSAE frequency was well-explained by ideal MHD theory without introducing non-perturbative energetic ion effects. The minimum value of RSAE frequency in the sweeping phase agrees well with GAM frequency. Nonlinear interaction between the RSAE and GAM generates a lot of driven modes. In thus produced low density RS configuration, bulk ion temperature in the plasma center T_(io) starts to increase linearly in time for more than 10 times of global energy confinement time just after the local minimum of the rotational transform has passed through the particular rational value τ/2π=1/3. When energetic ion driven AEs and GAM are reexcited appreciably, T_(io) decreases with slower time scale than that of the rise. During the rising phase of T_(io) , plasma potential measured by heavy ion beam probe becomes deeper in the plasma core region. Then, it becomes shallow in the decay phase of T_(io).
机译:在大型螺旋装置(LHD)中,通过强烈的反中性束(NB)电流驱动形成具有非单调旋转变换轮廓的反向磁剪切(RS)配置。在RS配置螺旋等离子体中,确定了n = 1环形模数的反向剪切Alfven本征模(RSAE)以及n = 0的高能离子驱动测地声模(GAM)。理想的MHD理论很好地解释了RSAE频率的时间扫描,而没有引入非扰动的高能离子效应。扫描阶段的RSAE频率最小值与GAM频率非常吻合。 RSAE和GAM之间的非线性交互会产生许多驱动模式。在如此产生的低密度RS构型中,刚好在旋转变换的局部最小值经过特定的正则之后,等离子体中心T_(io)中的体离子温度开始随时间线性增长,超过了全局能量限制时间的10倍以上。值τ/2π= 1/3。当高能离子驱动的AE和GAM重新激发时,T_(io)的下降时间尺度比上升时间慢。在T_(io)的上升阶段,通过重离子束探针测量的等离子体电势在等离子体核心区域变得更深。然后,在T_(io)的衰减阶段变浅。

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