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Fast ion absorption of the high harmonic fast wave in the National Spherical Torus Experiment

机译:国家球形圆环实验中高谐波快波的快速离子吸收

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Ion absorption of the high harmonic fast wave in a spherical torus [Y.-K. M. Peng , Nucl. Fusion 26, 769 (1986)] is of critical importance to assessing the viability of the wave as a means of heating and driving current. Analysis of recent National Spherical Torus Experiment [M. Ono , Nucl. Fusion 40, 557 (2000)] shots has revealed that under some conditions when neutral beam and rf power are injected into the plasma simultaneously, a fast ion population with energy above the beam injection energy is sustained by the wave. In agreement with modeling, these experiments find the rf-induced fast ion tail strength and neutron rate at lower B-fields to be less enhanced, likely due to a larger beta profile, which promotes greater off-axis absorption where the fast ion population is small. Ion loss codes find the increased loss fraction with decreased B insufficient to account for the changes in tail strength, providing further evidence that this is a rf interaction effect. Though greater ion absorption is predicted with lower k(parallel to), surprisingly little variation in the tail was observed, along with a neutron rate enhancement with higher k(parallel to). Data from the neutral particle analyzer, neutron detectors, x-ray crystal spectrometer, and Thomson scattering are presented, along with results from the TRANSP [R. J. Hawryluk, Physics of Plasmas Close to Thermonuclear Conditions 1, 19 (1981); J. P. H. E. Ongena , Fusion Technol. 33, 181 (1998)] transport analysis code, ray-tracing codes HPRT [J. Menard , Phys. Plasmas 6, 2002 (1999)], and CURRAY [T. K. Mau , RF Power in Plasmas: 13th Topical Conference (1999), p. 148], full-wave code AORSA [E. F. Jaeger , RF Power in Plasmas: 14th Topical Conference, 2001, p. 369], quasilinear code CQL3D [R. W. Harvey , in Proceedings of the IAEA TCM on Advances in Simulation and Modeling of Thermonuclear Plasmas, 1992], and ion loss codes EIGOL [D. S. Darrow , in Proceedings of the 6th IAEA TCM on Energetic Particles in Magnetic Confinement Systems, 2000, p. 109] and CONBEAM [J. Egedal , Phys. Plasmas 10, 2372 (2003)]. (C) 2004 American Institute of Physics.
机译:球形圆环中高次谐波快速波的离子吸收[Y.-K.彭(M. Fusion 26,769(1986)]对于评估电波作为加热和驱动电流手段的可行性至关重要。最近的国家球形圆环实验分析[M.小野Fusion 40,557(2000)]的镜头显示,在某些条件下,当中性束和rf功率同时注入等离子体时,该波会维持能量高于束注入能的快速离子种群。与建模相一致,这些实验发现,在较低B场下,射频诱导的快速离子尾部强度和中子速率增强的幅度较小,这可能是由于较大的β谱,从而促进了快速离子种群所在的更大的离轴吸收。小。离子损失代码发现损失分数随B降低而增加,不足以说明尾强度的变化,这进一步证明了这是rf相互作用效应。尽管预计在较低的k(平行)下会有更大的离子吸收,但是令人惊讶的是,尾部几乎没有变化,而较高的k(平行)则中子速率增强。给出了来自中性粒子分析仪,中子探测器,X射线晶体光谱仪和Thomson散射的数据,以及来自TRANSP的结果。 J. Hawryluk,接近热核条件的等离子体物理学,第19期,1981年; J.P.H.E.Ongena,融合技术。 33,181(1998)]传输分析代码,射线追踪代码HPRT [J.梅纳德Plasmas 6,2002(1999)]和CURRAY [T. K. Mau,“等离子体中的射频功率:第13届主题会议(1999),第2页”。 148],全波代码AORSA [E. F. Jaeger,“等离子体中的射频功率”:第14届主题会议,2001年,第1页。 369],准线性代码CQL3D [R. W. Harvey,在IAEA TCM会议论文集《热核等离子体的模拟和建模进展》(1992年)和离子损失代码EIGOL [D. S. Darrow,在《国际原子能机构第六次中医药关于磁约束系统中高能粒子的研究》,2000年,第1页。 109]和CONBEAM [J. Egedal,物理学。 Plasmas 10,2372(2003)。 (C)2004美国物理研究所。

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