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High resolution measurements of neutral density and ionization rate in the main chamber of the Alcator C-Mod tokamak

机译:高分辨率测量Alcator C-Mod托卡马克主室中的中性密度和电离率

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Recent theoretical and experimental work has focused on the importance of neutrals in the edge dynamics of Alcator C-Mod plasmas. Two new high resolution detectors have been installed on the Alcator C-Mod tokamak to measure the neutral density and ionization rate near the edge of the discharge in the main chamber. The detectors consist of a 20 channel photodiode array which views the plasma tangentially 12.5 cm below the outer midplane, and 10 cm above the inner midplane, with a nominal radial resolution of 2 and 3 mm, respectively. The spectral bandwidth is limited by a filter with a very narrow band around the neutral deuterium Lyman alpha wavelength (1215 Angstrom), The local emissivity is then obtained via a standard Abel inversion of the absolutely calibrated brightness profile, Employing well-known branching ratios, and using measured local electron density and temperature, we therefore, infer the neutral density and ionization rate with similar radial resolution. We have observed that both Lyman alpha emissivity and ionization rate are usually peaked near the separatrix with a full width, half-maximum between 1 and 2 cm, The neutral density was found to drop rapidly with decreasing minor radius, from 2-3 x 10(17)/m(3) (5-10 mm outside the separatrix) to 1-2 x 10(16)/m(3) (5-10 mm inside the separatrix) for a line averaged density of 2.0 x 10(20)/m(3), Variations in ionization rate and neutral density from low to high confinement mode (L and H mode) are also discussed. (C) 2001 Elsevier Science B.V, All rights reserved. [References: 6]
机译:最近的理论和实验工作集中在Alcator C-Mod等离子体的边缘动力学中中性的重要性。 Alcator C-Mod托卡马克上已安装了两个新的高分辨率探测器,以测量主腔室放电边缘附近的中性密度和电离率。检测器由一个20通道光电二极管阵列组成,该阵列在外中平面以下12.5 cm和内中平面以上10 cm切向观察等离子体,其径向标称分辨率分别为2和3 mm。光谱带宽受到中性氘莱曼α波长(1215埃)附近非常窄带的滤光片的限制,然后通过使用已知的分支比,通过绝对校准的亮度分布的标准Abel求逆获得局部发射率,并使用测得的局部电子密度和温度,我们以类似的径向分辨率推断出中性密度和电离速率。我们已经观察到,Lymanα的发射率和电离率通常在分离线附近达到峰值,全宽在1至2 cm之间,为半最大值,中间密度随着小半径的减小而迅速下降,从2-3 x 10 (17)/ m(3)(在分隔线外5-10毫米)至1-2 x 10(16)/ m(3)(在分隔线内5-10毫米),线平均密度为2.0 x 10( 20)/ m(3),还讨论了电离速率和中性密度从低限制模式到高限制模式(L和H模式)的变化。 (C)2001 Elsevier Science B.V,保留所有权利。 [参考:6]

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