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Experimental validation of non-uniformity effect of the radial electric field on the edge transport barrier formation in JT-60U H-mode plasmas

机译:JT-60U H型等离子体中径向电场对边缘传输势垒形成的非均匀效应的实验验证

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摘要

The turbulent structure formation, where strongly-inhomogeneous turbulence and global electromagnetic fields are self-organized, is a fundamental mechanism that governs the evolution of high-temperature plasmas in the universe and laboratory (e.g., the generation of edge transport barrier (ETB) of the H-mode in the toroidal plasmas). The roles of inhomogeneities of radial electric field (Er) are known inevitable. In this mechanism, whether the first derivative of Er (shear) or the second derivative of Er (curvature) works most is decisive in determining the class of nontrivial solutions (which describe the barrier structure). Here we report the experimental identification of the essential role of the Er-curvature on the ETB formation, for the first time, based on the high-spatiotemporal resolution spectroscopic measurement. We found the decisive importance of Er-curvature on ETB formation during ELM-free phase, but there is only a low correlation with the Er-shear value at the peak of normalized ion temperature gradient. Furthermore, in the ELMing phase, the effect of curvature is also quantified in terms of the relationship between pedestal width and thickness of the layer of inhomogeneous Er. This is the fundamental basis to understand the structure of transport barriers in fusion plasmas.
机译:湍流结构的形成是强烈不均匀的湍流和整体电磁场是自组织的,是控制宇宙和实验室中高温等离子体的演变的基本机制(例如,形成边缘传输势垒(ETB)环形等离子体中的H模式)。众所周知,径向电场(Er)的不均匀作用是不可避免的。在这种机制中,Er(剪切)的一阶导数或Er(曲率)的二阶导数最能决定非平凡解的类型(描述势垒结构)。在这里,我们首次基于高时空分辨率光谱测量结果,对Er曲率对ETB形成的重要作用进行了实验鉴定。我们发现,在无ELM阶段,Er曲率对ETB的形成具有决定性的重要性,但与归一化离子温度梯度峰值处的Er剪切值之间的相关性较低。此外,在ELMing阶段,还根据基座宽度和不均匀Er层的厚度之间的关系来量化曲率的影响。这是了解聚变等离子体中运输壁垒结构的基本基础。

著录项

  • 期刊名称 Scientific Reports
  • 作者

    K. Kamiya; K. Itoh; S.-I. Itoh;

  • 作者单位
  • 年(卷),期 -1(6),-1
  • 年度 -1
  • 页码 30585
  • 总页数 7
  • 原文格式 PDF
  • 正文语种
  • 中图分类
  • 关键词

  • 入库时间 2022-08-21 10:58:23

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