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首页> 外文期刊>Plasma physics and controlled fusion >Production and confinement characteristics of ICRF-accelerated energetic ions in JT-60U negative-shear plasmas
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Production and confinement characteristics of ICRF-accelerated energetic ions in JT-60U negative-shear plasmas

机译:JT-60U负剪切等离子体中ICRF加速的高能离子的产生和限制特征

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摘要

Characteristics of energetic ion tail formation during the second-harmonic ion cyclotron range of frequency (2 omega(CH) ICRF) heating and confinement of tail ions were investigated in negative magnetic shear plasmas on JT-60U. Charge-exchange neutral particle measurements show significantly lower tail temperature in negative-shear plasmas than those in positive-shear plasmas. The tail temperature in negative-shear plasmas increases with plasma current and shows improvement of energetic ion confinement. Charge-exchange neutral fluxes are also lower in negative-shear plasmas than in positive-shear plasmas. Meanwhile, tail ion stored energy is comparable between negative- and positive-shear plasmas. In order to understand these experimental results, simple modelled calculations were carried out with an orbit-following Monte Carlo (OFMC) code. The model calculations suggest that the ICRF power absorption is dominant near the 2 omega(CH) resonance in the negative-shear plasma and in the low-field side away from the 2 omega(CH) resonance in the positive-shear plasma. A larger scale length of pressure profile in the negative-shear plasma compensates for a lower density of tail ions than that in the positive-shear plasma. Accordingly, negative-shear plasmas can contain comparable stored energy of energetic tail ions to positive-shear plasmas. [References: 27]
机译:在JT-60U上的负磁切变等离子体中,研究了二次谐波离子回旋加速器在频率(2ω(CH)ICRF)加热和尾离子约束下的高能离子尾部形成特性。电荷交换中性粒子的测量结果显示,负剪切等离子体的尾部温度明显低于正剪切等离子体的尾部温度。负剪切等离子体中的尾部温度随等离子体电流而增加,并显示出高能离子约束的改善。负剪切等离子体中的电荷交换中性通量也比正剪切等离子体中的低。同时,尾离子存储的能量在负剪切等离子体和正剪切等离子体之间是可比的。为了理解这些实验结果,使用遵循蒙特卡洛(OFMC)编码的轨道进行了简单的建模计算。模型计算表明,ICRF功率吸收在负剪切等离子体中的2 omega(CH)共振附近和在低磁场侧占主导地位,而在正剪切等离子体中远离2 omega(CH)共振的低场侧占主导。与正剪切等离子体相比,负剪切等离子体中较大的压力曲线刻度长度补偿了较低的尾离子密度。因此,负剪切等离子体可以包含与正剪切等离子体相当的高能尾离子存储能量。 [参考:27]

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