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洞态Ar原子K_α和K_β伴线和超伴线的理论计算
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作者 马堃 焦铮 +3 位作者 蒋峰建 叶剑锋 吕海江 陈展斌 《物理学报》 SCIE EI CAS CSCD 北大核心 2018年第17期87-93,共7页
基于全相对论多组态Dirac-Fock方法,对L壳层旁观空穴下Ar原子退激衰变辐射K-X射线K_(α1,2)(K→L_(3,2))和K_(β1,3)(K→M_(3,2))的6908条伴线和超伴线跃迁能、跃迁概率进行了系统计算,计算结果与文献已有数据比较具有很好的一致性.通过... 基于全相对论多组态Dirac-Fock方法,对L壳层旁观空穴下Ar原子退激衰变辐射K-X射线K_(α1,2)(K→L_(3,2))和K_(β1,3)(K→M_(3,2))的6908条伴线和超伴线跃迁能、跃迁概率进行了系统计算,计算结果与文献已有数据比较具有很好的一致性.通过对(K^(-1)L^(-1),l=0-8)伴线和(K^(-2)L^(-l),l=0-8)超伴线跃迁谱线卷积得了其合成谱,给出了L壳层不同空穴数下K-X射线伴线和超伴线的平均能量和平均跃迁强度.结果表明,退激辐射X射线能量以及能移与L壳层空穴个数呈现明显的线性关系.基于结论,进一步给出了跃迁能移与L壳层空穴个数之间的关系表达式.研究结果可以为解释离子、原子碰撞过程中产生的X射线谱提供重要的理论支持. 展开更多
关键词 原子 伴线 超伴线 X射线
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锂洞原子双激发态的鞍点能量计算
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作者 张茹 刘刚 焦荣珍 《原子与分子物理学报》 CAS CSCD 北大核心 2002年第4期527-530,共4页
采用鞍点截断变分方法和鞍点复数转动技术 ,计算和分析了锂洞原子双激发共振态 [1s(2s2p) 3 P]2 P0 的鞍点能量和波函数。
关键词 双激发态 计算 原子 鞍点变分法 鞍点能量
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L壳层双洞态氩离子的退激发及末电离态分布的研究 被引量:1
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作者 王向丽 胡宏伟 董晨钟 《原子与分子物理学报》 CAS CSCD 北大核心 2008年第3期493-498,共6页
基于洞原子退激发的辐射-俄歇级联退激发模型(radiative-Auger cascade model简称RAC模型),本文详细研究了Ar2+(2s-2)、Ar2+(2s-12p-1)和Ar2+(2p-2)三种离子的退激发过程及其末电离态离子分布,讨论了末电离态离子分布随初态洞的深浅变... 基于洞原子退激发的辐射-俄歇级联退激发模型(radiative-Auger cascade model简称RAC模型),本文详细研究了Ar2+(2s-2)、Ar2+(2s-12p-1)和Ar2+(2p-2)三种离子的退激发过程及其末电离态离子分布,讨论了末电离态离子分布随初态洞的深浅变化的规律.结果表明:随着初态洞分布的变浅,退激发过程变简单,退激发后产生的高离化度离子分布降低,低离化度离子分布增大. 展开更多
关键词 原子(或离子) RAC模型 退激发树 末电离态离子分布
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Observation of Inception of Sheet Cavitation from Free Nuclei 被引量:5
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作者 Wakana TSURU Takafumi KONISHI +1 位作者 Satoshi WATANABE Shin-ichi TSUDA 《Journal of Thermal Science》 SCIE EI CAS CSCD 2017年第3期223-228,共6页
Prediction of inception of sheet cavitation on solid walls has been recognized to be very difficult, since it is significantly affected by the boundary layer flow characteristics, the population of free nuclei, the nu... Prediction of inception of sheet cavitation on solid walls has been recognized to be very difficult, since it is significantly affected by the boundary layer flow characteristics, the population of free nuclei, the nuclei held in the wall roughness, the amount of dissolved air in liquid and so on. It has not sufficiently been made clear how the inception is affected by the conditions of water qualities and background flow characteristics. In this study, high speed observation of inception of sheet cavity from free nuclei is conducted for a two-dimensional convergent-divergent nozzle flow, where the sheet cavity forms just downstream of the nozzle throat. The effects of the amount of dissolved air and the free stream velocity on the inception process of sheet cavitation is examined. In addition, the bubble nuclei density, which is well known to be important factor for cavitation inception, is passively controlled by the filter installed in the tunnel. From the observations, it is confirmed that the nuclei number density significantly affects the formation of sheet cavity rather than the other two parameters. In conditions with large nuclei number density, the sheet cavity does not form, and bubbly cavitation appears instead. In the case with small nuclei number density, the sheet cavity forms from a single flowing nucleus and develops streamwisely and spanwisely. In the conditions with medium nuclei number density, the sheet cavity also forms but is shorter/narrower streamwisely/spanwisely, due to interaction of other nuclei flowing near the formed sheet cavity. 展开更多
关键词 Cavitation inception Sheet cavity Nuclei distribution Dissolved air
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