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Observation of an impurity hole in a plasma with an ion internal transport barrier in the Large Helical Device

机译:大型螺旋装置中带有离子内部传输势垒的等离子体中杂质孔的观察

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摘要

Extremely hollow profiles of impurities (denoted as “impurity hole”) are observed in the plasma with a steep gradient of the ion temperature after the formation of an internal transport barrier (ITB) in the ion temperature transport in the Large Helical Device [A. Iiyoshi et al., Nucl. Fusion 39, 1245 (1999)]. The radial profile of carbon becomes hollow during the ITB phase and the central carbon density keeps dropping and reaches 0.1%?0.3% of plasma density at the end of the ion ITB phase. The diffusion coefficient and the convective velocity of impurities are evaluated from the time evolution of carbon profiles assuming the diffusion and the convection velocity are constant in time after the formation of the ITB. The transport analysis gives a low diffusion of 0.1?0.2 m2/s and the outward convection velocity of ~1 m/s at half of the minor radius, which is in contrast to the tendency in tokamak plasmas for the impurity density to increase due to an inward convection and low diffusion in the ITB region. The outward convection is considered to be driven by turbulence because the sign of the convection velocity contradicts the neoclassical theory where a negative electric field and an inward convection are predicted.
机译:在大型螺旋装置中,在离子温度传输中形成内部传输势垒(ITB)之后,在等离子体中观察到杂质的中空轮廓(称为“杂质孔”),且离子温度具有陡峭的梯度。 Iiyoshi et al。,Nucl。 Fusion 39,1245(1999)]。碳的径向分布在ITB相期间变为空心,并且中心碳密度持续下降,并在离子ITB相结束时达到等离子体密度的0.1%〜0.3%。从碳分布的时间演变来评估杂质的扩散系数和对流速度,前提是假设在ITB形成后扩散和对流速度在时间上是恒定的。输运分析得出在较小半径的一半处的低扩散为0.1?0.2 m2 / s,向外对流速度为〜1 m / s,这与托卡马克等离子体中杂质浓度由于以下原因而增加的趋势相反:在ITB区域内向内对流和低扩散。认为对流是由湍流驱动的,因为对流速度的符号与新古典理论相矛盾,在新古典理论中,预测了负电场和向内对流。

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