HL-2A托卡马克边界等离子体数值模拟及非日冕平衡条件下的杂质辐射问题研究

对边界层等离子体中常见的物理问题，从两点模型到二维流体描述。从原子分子物理过程到杂质的输运和辐射等进行了系统的归纳和总结，特别是对等离子体不同参数运行区如鞘层限制参数区、传导限制参数区以及脱靶参数区等的一维流体描述，在参阅相关文献的基础上使用一定的假设条件进行了简单推导。分别阐述了它们的特点。     

Evolution of the high-field-side radiation belts during the neon seeding plasma discharge in EAST tokamak

Divertor detachment achieved by injecting impurities or increasing density is always accompanied with various local radiation phenomena in the boundary or core plasma. This paper presents the formation and evolution of the high-field-side (HFS) radiation belts during the neon seeding plasma discharge in upper single null configuration with two directions of toroidal magnetic field in EAST tokamak. The neon mixed with deuterium seeding can induce the divertor detachment with strong radiation belts in the HFS scrape-off layer (SOL) region. With the increase of the radiation power, the plasma discharge will transit from H-mode to L-mode, and meanwhile the radiation belts move away from the near X-point to HFS SOL. When the radiation power is high enough, the radiation belts begin to move further to the other X-point along the HFS SOL, and even cause plasma disruption. The results indicate that the behavior of the radiation belts is related to the radiation power, plasma confinement performance and state of divertor detachment, which is useful for developing better feedback control methods to achieve high-performance radiative divertor operation mode.     

非磁化等离子体和磁化等离子体的电磁辐射特性研究

本文研究非磁化和磁化双MAXWELL分布等离子体的电磁不稳定性色散方程和电磁辐射增长率.结果表明,非磁化等离子体不能辐射出电磁波,而磁化等离子体能够辐射出电磁波.并分析讨论了磁化等离子体在不同参数下的电磁辐射增长率随辐射频率、等离子体密度和温度的变化.     

喷气Z箍缩X光辐射信号分析

 在清华大学喷气Z箍缩平台上进行了对Ne气的箍缩软X射线诊断工作。该喷气装置由4个充电至23 kV的电容器并联组成,总储能4.5 kJ,放电电流峰值210 kA,上升沿2.5 ms。实验中通过观测放电电流微分信号来观测箍缩聚焦点的位置（波形的下凹尖峰点）,此尖峰也是X光辐射的时间分辨点。利用响应时间为亚ns量级的光敏半导体探测器(PIN)探头获得了Ne气箍缩时等离子体发出的软X射线信号,X光辐射出现在放电电流微分信号突变点附近。一般来说,多次箍缩会导致多次的X光辐射输出,实验中的X光脉冲实际为多个等离子热点辐射叠加的结果,单次箍缩所产生的X光辐射比多次箍缩所产生的X光辐射要强。对每次箍缩来说,单个X光脉冲信号比多个X光脉冲信号的幅值要大。     

喷气Z箍缩X光辐射信号分析

在清华大学喷气Z箍缩平台上进行了对Ne气的箍缩软X射线诊断工作。该喷气装置由4个充电至23 kV的电容器并联组成,总储能4.5 kJ,放电电流峰值210 kA,上升沿2.5 ms。实验中通过观测放电电流微分信号来观测箍缩聚焦点的位置（波形的下凹尖峰点）,此尖峰也是X光辐射的时间分辨点。利用响应时间为亚ns量级的光敏半导体探测器(PIN)探头获得了Ne气箍缩时等离子体发出的软X射线信号,X光辐射出现在放电电流微分信号突变点附近。一般来说,多次箍缩会导致多次的X光辐射输出,实验中的X光脉冲实际为多个等离子热点辐射叠加的结果,单次箍缩所产生的X光辐射比多次箍缩所产生的X光辐射要强。对每次箍缩来说,单个X光脉冲信号比多个X光脉冲信号的幅值要大。     

Dynamic optogalvanic effect in a neon plasma

This paper presents a model of the dynamic optogalvanic effect. On the basis of this model an explanation is given for the experimental data obtained in a neon gas-discharge plasma.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 2, pp. 84–89, February, 1987.     

On the thermophoresis in dense dust structures in neon plasma

Numerical study of the effect of dust particle concentration on the thermophoretic force acting on a dust particle inside a dust structure in plasma has been carried out. The experimental data on the formation of voids in dust structures formed by 2.55 μm dust particles in a glow dc discharge in neon have been used. The simulation has been performed using the diffusion-drift model with taking into account joule heating of discharge. The dependence of the thermophoretic force acting on a dust particle in a dust structure on the ratio of atom mean free path to the distance between the adjacent particles in the dust structure has been obtained.     

Role of neon in a decaying high-purity helium plasma

The evolution of the electron and atomic and molecular metastable densities and the radiation of the decaying plasma of helium with a 10^–5-fraction of neon additive is experimentally studied. A model of elementary processes in He–Ne plasma is constructed, which describes the formation and destruction of HeNe⁺ and Ne₂ ⁺ molecular ions and their contribution to the formation of the afterglow spectrum by the electronion recombination. The various criteria influence of neon on the parameters of the decaying plasma are studied. The possibility of determining the amount of neon in helium by measuring the relative intensities of helium molecular bands and neon spectral lines in the afterglow is considered.     

Analysis of time phase of characteristic radiation in plasma induced by laser ablating aluminum

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Investigation of the electron energy distribution function in a neon afterglow plasma

Probe measurements of the electron energy distribution function conducted in a neon afterglow plasma showed substantial deviations from a maxwellian distribution function in the high energy range. The differences result from Penning ionization and electron-metastable atom superelastic collisions.     

Tunable XUV radiation generated by nonresonant frequency tripling in neon

Nonresonant frequency tripling of ultraviolet (UV) radiation (λ_uv = 216–223 nm, generated by sum frequency mixing of the outputs of a frequency doubled pulsed dye laser and of the Nd-YAG pump laser) generates in neon coherent light in the extreme ultraviolet (XUV). The XUV radiation is tunable in spectral regions of negative dispersion λ_xuv = 72.05- 73.58 nm and λ_xuv = 74.3–74.36 nm at the high energy side of the transitions $\text{2p-3s′[}\text{built1}\text{2}\text{, 1]}$ and $\text{2p-3s[}\text{built3}\text{2}\text{, 1]}$. At UV input powers of 0.1-0.3 MW the generated XUV power was typically P_xuv = 0.1-0.4 W (1.5–6 x 10⁸ photons/pulse). Since present UV dye laser systems provide at λ_uv pulse powers of almost 1 MW the XUV output could easily be increased by more than one order of magnitude.