High-density plasma with internal diffusion barrier in the Large Helical Device

High-density plasma with internal diffusion barrier in the Large Helical Device
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DOI:
10.1088/0029-5515/49/8/085002
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发表时间:
2009-07
期刊:
影响因子:
3.3
通讯作者:
R. Sakamoto;M. Kobayashi;J. Miyazawa;S. Ohdachi;H. Yamada;H. Funaba;M. Goto;S. Masuzaki;T. Morisaki;I. Yamada;K. Narihara;K. Tanaka;S. Morita;K. Ida;S. Sakakibara;Y. Narushima;K. Watanabe;Y. Suzuki;N. Ashikawa;Y. Nagayama;B. Peterson;M. Shoji;C. Suzuki;M. Tokitani;S. Yoshimura;N. Ohyabu;A. Komori;O. Motojima
R. Sakamoto;M. Kobayashi;J. Miyazawa;S. Ohdachi;H. Yamada;H. Funaba;M. Goto;S. Masuzaki;T. Morisaki;I. Yamada;K. Narihara;K. Tanaka;S. Morita;K. Ida;S. Sakakibara;Y. Narushima;K. Watanabe;Y. Suzuki;N. Ashikawa;Y. Nagayama;B. Peterson;M. Shoji;C. Suzuki;M. Tokitani;S. Yoshimura;N. Ohyabu;A. Komori;O. Motojima
中科院分区:
物理与天体物理1区
文献类型:
--
作者:
R. Sakamoto;M. Kobayashi;J. Miyazawa;S. Ohdachi;H. Yamada;H. Funaba;M. Goto;S. Masuzaki;T. Morisaki;I. Yamada;K. Narihara;K. Tanaka;S. Morita;K. Ida;S. Sakakibara;Y. Narushima;K. Watanabe;Y. Suzuki;N. Ashikawa;Y. Nagayama;B. Peterson;M. Shoji;C. Suzuki;M. Tokitani;S. Yoshimura;N. Ohyabu;A. Komori;O. Motojima

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在大螺旋装置(LHD)的螺旋偏滤器中发现了一种有吸引力的高密度运行机制,即所谓的内扩散势垒(IDB)。IDB的特点是陡峭的密度梯度和等离子体轮廓被IDB分为高密度的核心等离子体和低密度的地幔等离子体。IDB使堆芯等离子体能够进入高密度/高压区。可达到的中心密度超过1 × 1021 m−3,中心压力达到大气压的1.5倍。堆芯芯弹丸加料对于IDB的形成是绝对必要的,并且通过采用密集的多弹丸注入可重复地获得。在IDB堆芯等离子体中,尽管存在高密度和陡峭的密度梯度,但粒子扩散系数保持在相当低的水平,0.05 m2 s-1,而没有观察到向内的粒子对流速度。
An attractive high-density operational regime which is a so-called internal diffusion barrier (IDB) has been discovered in a helical divertor configuration on the Large Helical Device (LHD). The IDB is characterized by steep density gradients and the plasma profile is divided by the IDB into a high-density core plasma and a low density mantle plasma. The IDB enables the core plasma to access the high-density/high-pressure regime. The attainable central density exceeds 1 × 1021 m−3 and the central pressure reaches ≈1.5 times atmospheric pressure. Core pellet fuelling is absolutely essential for the IDB formation and it is reproducibly obtained by employing intensive multiple-pellet injection. In the IDB core plasma, the particle diffusion coefficient is kept at a considerably low level, 0.05 m2 s−1, in spite of high-density and steep-density gradients whereas an inward particle convection velocity is not observed.