A. Henriquez, H. Bhuyan, M. Favre, H. Chuaqui, E. Wyndham
{"title":"Temporal and spatial evolution of carbon ion beam emission in plasma focus discharges","authors":"A. Henriquez, H. Bhuyan, M. Favre, H. Chuaqui, E. Wyndham","doi":"10.1109/PLASMA.2008.4590965","DOIUrl":null,"url":null,"abstract":"Summary form only given. In plasma focus (PF) a high density, high temperature, short duration Z-pinch like plasma column is formed, following a radial compression phase. The PF is a well known source of energetic ion beams, of characteristic energy from hundreds of keV to tens of MeV. Several theoretical and computational models have been developed in an attempt to explain the ion production and acceleration mechanism in PF discharges. Despite this theoretical effort, a complete explanation of the ion emission mechanism is still not available. We have performed a detailed investigation on the time evolution and angular distribution of PF ion beams. We have previously characterized the main features of ion beam emission in a low energy, 1.8 kJ, 160 kA Mather type PF device, operating in methane. In the present investigation axial and radial biased Faraday cup ion probes, which are also sensitive to XUV radiation, were used simultaneously in conjunction with a radial X-ray detector to correlate the ion beam emission with the different stages in the PF dynamics. We have observed that the ion beams emitted radially are mostly associated with the radial compression phase of the PF discharge, prior to the formation of a Z-pinch like plasma column. At this stage the ion beams composition is dominated by C+2 ions. At later times, around the maximum compression phase, the axial emission becomes dominant and the ion beam composition is found to be mainly C+4 and C+5 ions. In general, the axial ion beam emission is found to be of much higher characteristic energy and flux than the radial emission. These results indicate that no unique mechanism for ion beam emission in PF can be assumed. Based on the time correlations and measured properties of the ion beams, the plasma conditions at the time of the different stages in the ion emission will be discussed, in order to assess the validity of current PF ion beam emission models, which account for different properties of the beams, such as characteristic energy scaling and angular distribution.","PeriodicalId":6359,"journal":{"name":"2008 IEEE 35th International Conference on Plasma Science","volume":"PE-2 1","pages":"1-1"},"PeriodicalIF":0.0000,"publicationDate":"2008-06-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2008 IEEE 35th International Conference on Plasma Science","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/PLASMA.2008.4590965","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Summary form only given. In plasma focus (PF) a high density, high temperature, short duration Z-pinch like plasma column is formed, following a radial compression phase. The PF is a well known source of energetic ion beams, of characteristic energy from hundreds of keV to tens of MeV. Several theoretical and computational models have been developed in an attempt to explain the ion production and acceleration mechanism in PF discharges. Despite this theoretical effort, a complete explanation of the ion emission mechanism is still not available. We have performed a detailed investigation on the time evolution and angular distribution of PF ion beams. We have previously characterized the main features of ion beam emission in a low energy, 1.8 kJ, 160 kA Mather type PF device, operating in methane. In the present investigation axial and radial biased Faraday cup ion probes, which are also sensitive to XUV radiation, were used simultaneously in conjunction with a radial X-ray detector to correlate the ion beam emission with the different stages in the PF dynamics. We have observed that the ion beams emitted radially are mostly associated with the radial compression phase of the PF discharge, prior to the formation of a Z-pinch like plasma column. At this stage the ion beams composition is dominated by C+2 ions. At later times, around the maximum compression phase, the axial emission becomes dominant and the ion beam composition is found to be mainly C+4 and C+5 ions. In general, the axial ion beam emission is found to be of much higher characteristic energy and flux than the radial emission. These results indicate that no unique mechanism for ion beam emission in PF can be assumed. Based on the time correlations and measured properties of the ion beams, the plasma conditions at the time of the different stages in the ion emission will be discussed, in order to assess the validity of current PF ion beam emission models, which account for different properties of the beams, such as characteristic energy scaling and angular distribution.
只提供摘要形式。在等离子体聚焦(PF)中,在径向压缩阶段之后,形成高密度、高温、短持续时间的z捏状等离子体柱。PF是一种众所周知的高能离子束源,特征能量从数百keV到数十MeV不等。为了解释PF放电中的离子产生和加速机制,已经建立了几个理论和计算模型。尽管在理论上做出了努力,但对离子发射机制的完整解释仍然不可用。我们对PF离子束的时间演化和角度分布进行了详细的研究。我们以前已经描述了在甲烷中工作的低能量,1.8 kJ, 160 kA Mather型PF装置中离子束发射的主要特征。在本研究中,轴向和径向偏置法拉第杯离子探针也对XUV辐射敏感,同时与径向x射线探测器结合使用,将离子束发射与PF动力学的不同阶段相关联。我们已经观察到,离子束径向发射主要与PF放电的径向压缩阶段有关,在形成Z-pinch样等离子体柱之前。在这个阶段,离子束的组成主要是C+2离子。在后期,在最大压缩阶段左右,轴向发射成为主导,离子束成分主要是C+4和C+5离子。一般来说,发现轴向离子束发射比径向发射具有更高的特征能量和通量。这些结果表明,不能假设PF中离子束发射的独特机制。基于离子束的时间相关性和测量性质,讨论了离子束发射不同阶段时的等离子体条件,以评估当前PF离子束发射模型的有效性,这些模型考虑了离子束的不同特性,如特征能量缩放和角度分布。