等离子体屏蔽效应对类氢离子能级结构和辐射跃迁性质的影响

在Debye-Hückel屏蔽近似下,基于相对论Dirac-Fock方法,发展了包括等离子体屏蔽效应的自洽场计算程序.使用该程序研究了等离子体屏蔽效应对类氢离子能级结构和辐射跃迁性质的影响.结果表明,当原子处于等离子体环境中,所有束缚态能级向连续态移动, 移动量随着屏蔽长度的减小而增大.振子强度随屏蔽长度的变化也表现出了相同的规律.进一步分析了相对论效应和等离子体屏蔽效应的耦合,发现对于中Z元素,相对论效应和等离子体屏蔽效应存在较强的耦合.讨论了等离子体屏蔽效应对原子精细结构能级的影响.计算发现,由于等离子体屏蔽效应,原子的能级次序发生了变化,κ简并被消除. 关键词： 等离子体屏蔽 Debye-Hückel 模型 能级结构 跃迁概率     

磁光光子晶体结构的法拉第效应增强

在超薄薄膜的基础上,基于时域有限差分法原理,利用FDTD Solutions仿真软件分别研究了基于两种多层膜结构和一种金属光栅结构的磁光光子晶体法拉第旋光效应。研究表明,多层膜结构的法拉第旋光效应增强原理为入射光在薄膜中心层的透射谱谐振,而金属光栅周期结构的法拉第效应增强是通过金属光栅激发表面等离子体实现的;在三种结构中,金属光栅周期结构具有更广的法拉第偏转角增强域。进一步通过参数优化,实现对金属光栅周期结构工作波长的可调节性研究,为薄膜型磁光器件设计提供了理论依据。     

温稠密等离子体中Al12+离子的光电离过程

本文采用多组态Dirac-Hartree-Fock方法研究了温稠密等离子体环境中Al12+离子的光电离过程. 等离子体效应采用SM屏蔽势来模拟(Stanton和Murillo在2015年提出). 计算中固定标度温度1.3eV,在强耦合等离子体环境下,研究了等离子体密度对能级,连续态波函数以及光电离截面的影响. 通过与相同等离子体条件下的Debye-Hückel模型势计算的光电离截面对比,发现两种模型对应的结果中未同时出现势形共振峰,这是由于本文采用的屏蔽模型包含等离子体简并、有限温度对动能的梯度修正和量子交换关联效应,对光电离截面的大小和共振结构具有显著影响.     

基于等离子体环境涨落的原子结构计算模型

本文将等离子体核聚变反应截面研究中利用等离子体环境涨落进行修正了的Debye-Hückel屏蔽势推广到计算等离子体中辐射离子束缚态的能级结构. 通过Tsallis参数q的变化,在等离子体辐射离子束缚态能级结构的计算中加入等离子体参数涨落的平均效应,即,等离子体动力学. 具体给出了利用修正的Debye-Hückel屏蔽势对类氦铝束缚态能级结构的计算结果. 结果表明基于这种修正的屏蔽势,自由电子的极化分布具有和线性Debye-Hückel屏蔽势不同的结构. 这种通过等离子体涨落分布对屏蔽势函数进 关键词： 等离子体中的原子结构 等离子体环境涨落 修正了的Debye-Hückel屏蔽势     

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介绍了HCSB TBM屏蔽块的初步设计,根据RCC-MR相关标准,在4种典型工况下对TBM屏蔽块的结构性能进行了分析和校核。计算结果表明：所有工况下的整体形变都较小,一次应力和二次应力均满足RCC-MR标准。     

HCSB TBM 屏蔽块初步设计与结构性能分析

介绍了HCSB TBM 屏蔽块的初步设计,根据RCC-MR 相关标准,在4 种典型工况下对TBM 屏蔽块的结构性能进行了分析和校核。计算结果表明：所有工况下的整体形变都较小,一次应力和二次应力均满足 RCC-MR 标准。     

等离子体屏蔽效应对类氢离子束缚态的影响

在Debye屏蔽近似下,通过求解Schrödinger方程,计算了处于等离子体中的类氢离子的束缚态能量本征值与本征函数. 研究了氢原子和类氢Fe25+离子的n l ( n =1-4, l = 0-3)态能级随Debye 屏蔽长度λ的变化规律. 进一步,分析了等离子体屏蔽效应随主量子数n及角量子数l的变化规律, 发现对于给定的l, 等离子体屏蔽效应随主量子数n的增加而增大;对于给定的n,等离子体屏蔽效应随角量子数l 的增大而减小. 最后,我们分析了等离子体环境中类氢等电子序列离子的能级和波函数随屏蔽参数λ的变化规律,发现随着原子序数增大,等离子体屏蔽效应的影响逐渐变小.     

磁化等离子体环境对氢原子能级结构的影响

本文通过非微扰求解薛定谔方程, 研究了强磁场磁化的等离子体环境中的原子能级结构和辐射动力学过程. 在较宽的磁场强度范围和等离子体屏蔽参数范围内, 给出了氢原子基态以及低激发态的能级、辐射跃迁能量和振子强度等重要的原子参数, 定量地描述了强磁场和等离子体屏蔽共同作用的综合效应. 相关的结果有助于增进对极端环境下原子光谱结构的认识, 在等离子体光谱诊断和天文光谱观测方面有一定的借鉴意义. 关键词： 强磁场 CWDVR谱方法 能级结构 振子强度     

纳秒脉冲激光诱导水等离子体屏蔽的实验研究

基于激光阴影法测量原理,建立了一个记录纳秒脉冲激光诱导等离子体屏蔽现象的实验光路系统,探索了一种等离子体屏蔽图像的记录方法,对纳秒脉冲激光诱导水击穿形成等离子体的现象进行了研究.记录了在不同能量状态下出现的激光诱导等离子体屏蔽图像,发现了激光诱导水介质的等离子体屏蔽效应随作用光能量呈增强的趋势,首次观测到了在纳秒脉冲激光作用下液体中出现的线型击穿现象.本文研究结果可为水下激光加工研究、医疗以及激光在液体中的传播特性研究提供实验依据.     

纳秒脉冲激光诱导水等离子体屏蔽的实验研究

基于激光阴影法测量原理,建立了一个记录纳秒脉冲激光诱导等离子体屏蔽现象的实验光路系统,探索了一种等离子体屏蔽图像的记录方法,对纳秒脉冲激光诱导水击穿形成等离子体的现象进行了研究.记录了在不同能量状态下出现的激光诱导等离子体屏蔽图像,发现了激光诱导水介质的等离子体屏蔽效应随作用光能量呈增强的趋势,首次观测到了在纳秒脉冲激光作用下液体中出现的线型击穿现象.本文研究结果可为水下激光加工研究、医疗以及激光在液体中的传播特性研究提供实验依据.     

Simulation of the electromagnetic characters of a Faraday-shielded antenna in a helicon wave plasma source

In this article, a structure that employs a Faraday shield between the Shoji antenna and the dielectric tube, which aims to reduce the dielectric wall sputtering, is investigated for the helicon wave plasma (HWP) sources. Faraday shield is usually used between the antenna and the reaction chamber to reduce the radiation from the high electromagnetic field generation, as well as to prevent the sputtering of the antenna material from polluting the reaction chamber during the discharge. Here, the influence of the Faraday shield on the longitudinal and radial electric field of the antenna is analysed through COMSOL Multiphysics^TM. Significant attenuations of both the longitudinal and radial fields are observed in the presence of the shield. In addition, by comparing the electric field distribution under two different shielding parameters, it is found that the shielding effects are not the same. Therefore, a detailed study of two kinds of design (pitch and gap) for the shield was carried out. The results show that the pitch has a little impact on the overall shielding effect when the gap is unaltered. The best shielding performance appears when we set the pitch at T of 8 and 10. In addition, the shielding effect also becomes worse as the gap increases while the pitch remains unchanged. A relatively good shielding effect can be produced by setting the gap to the value of 4–8 mm (a gap/pitch ratio of 2/15–4/15). This work provides a theoretical basis for designing a Faraday shield structure between the antenna and the dielectric tube, which is helpful to realize stable and controllable HWP discharges.     

Faraday shield effects on a half-turn loop antenna used for ICRFplasma heating

The characteristics of a half-turn loop antenna having a Faraday shield (used for ion-cyclotron RF plasma heating) have been systematically investigated. The main interest is to clarify the Faraday shield effects on the near-zone electric field distribution. It has been confirmed that, in the presence of the Faraday shield, undesirable field components are sufficiently suppressed, and the heating component E _y, which otherwise is strongly localized as an end effect, has been found to be distributed uniformly along the antenna in the case of a short electric length. It is found that the shielding strips should be uniformly distributed over the entire region around the half-turn loop antenna     

Faraday镜预转角对FMOCT输出光偏振态的影响

通过计算机仿真,运用琼斯矩阵理论分析了Faraday镜预转角对法拉第镜式光学电流互感器输出光偏振态的影响.实验测量了Faraday镜实际预转角的大小,测量了外磁场的改变对Faraday镜预转角的影响.外磁场的存在和变化使Faraday镜预转角偏离初始值,并使系统输出光由理想状态下的线偏振光退化成椭圆偏振光,并引起法拉第镜式光学电流互感器工作灵敏度和稳定性的下降.提出了用电磁屏蔽解决外界磁场影响的方法.     

Measurement of the effects of Faraday shields on ICRH antennacoupling

Compact loop antennas are being applied to several fusion experiments, including DIII-D, the Advanced Toroidal Facility, Tore Supra, and the Tokamak Fusion Test Reactor. Although individual configurations vary, all of these antennas generally comprise a current strap in a recessed box and a Faraday shield. The coupling characteristics of cavity antennas that have current straps with the previously evaluated cross-sectional shapes are tested with several Faraday shields. The coupling is purely a measure of the magnetic flux linkage at relevant ion-cyclotron resonance heating (ICRH) frequencies and does not include plasma spectral effects. Impedances and relative fields are measured for various combinations of the current strap and Faraday shield. The experiments show that the fractional reduction in the magnetic flux linkage to the plasma resulting from the addition of any particular Faraday shield is virtually independent of the shape of the current strap. This is true in spite of the fact that the same mechanism which is responsible for the reduction in flux is also responsible for a significant redistribution of the antenna current on the current strap. Thus the process of optimizing antennas is reduced to that of separately optimizing the current strap and Faraday shield     

The interrelation between the Faraday effect and the inverse Faraday effect in a magnetic medium and the terahertz inverse Faraday effect in single molecule magnets

The interrelation between the Faraday and the inverse Faraday effects when the magneto-dipole interaction of a sample with an electromagnetic wave is essential has been phenomenologically investigated. This investigation was carried out in the spirit of well-known Pitaevsky’s approach. The terahertz inverse Faraday effect in single molecule magnets has been theoretically studied, the conditions favorable for observing this effect have been formulated.     

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现有的法拉第屏蔽(FS)冷却结构无法满足未来EAST长脉冲稳态运行的要求,需要进行优化改进.通过理论和数值模拟方法,对FS原有冷却结构进行了优化设计,并获得了改进后FS冷却管道的流速和压力分布.通过比较不同进口条件下FS流体压降和结构温度分布情况,获得了适合优化后FS结构运行的流动参数,为未来ICRH天线FS的运行提供了理论指导.     

EAST ICRH天线法拉第屏蔽冷却结构优化

现有的法拉第屏蔽(FS)冷却结构无法满足未来EAST 长脉冲稳态运行的要求,需要进行优化改进。通过理论和数值模拟方法,对FS原有冷却结构进行了优化设计,并获得了改进后FS冷却管道的流速和压力分布。通过比较不同进口条件下FS流体压降和结构温度分布情况,获得了适合优化后FS结构运行的流动参数,为未来ICRH天线FS的运行提供了理论指导。     

Faraday Rotation of Overdense Magnetized Plasma

In this study, we investigate Faraday rotation of electromagnetic waves that are anomalously transmitted through an over‐dense magnetized plasma layer. Here, magnetized plasma indicates that the plasma layer is immersed in a uniform magnetic field. Firstly, normally opaque over‐dense magnetized plasma is shown to be transparent to obliquely incident electromagnetic waves. This high transparency can be achieved by providing conditions for resonant excitations of plasmonic modes. The resonant characteristics of the transmission coefficient of the considered structure are determined and discussed. The conditions under which the magnetized plasma behaves as a complete reflector are also obtained. Faraday rotation is shown to be enhanced under high transparency conditions. The reflected wave also exhibits Faraday rotation and is enhanced under total reflection conditions. (© 2015 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

Tests of an ICRH Resonant Cavity Launcher with Faraday Shield

A resonant cavity antenna designed to be suitable for ion cyclotron heating in a tokamak has been bench tested. This antenna is a "discrete element" circuit designed to launch the fast magnetosonic wave in a magnetized plasma. The resonant autotransformer design allows matching to the transmission-line impedance. The tuning and matching properties of this antenna have been compared with a simple computer model. The effective transmission of various Faraday shields has been determined by measuring the change in Q of the antenna system with and without the shield. The test results show that the antenna behaves as predicted by a simple computer model and that coolable Faraday shields with high RF transmission can be designed.     

Theory of the inverse Faraday effect in metals

An analytic expression is given for the inverse Faraday effect, i.e., for the magnetization occuring in a transparent medium exposed to a circularly polarized high-frequency electromagnetic wave. Using a microscopic approach based on the Drude approximation of a free-electron gas, the magnetization of the medium due to the inverse Faraday effect is identified as the result of microscopic solenoidal currents generated by the electromagnetic wave. In contrast to the better known phenomenological derivation, this microscopic treatment provides important information on the frequency dependence of the inverse Faraday effect.