利用类铜离子谱线诊断银等离子体电子密度

测量了激光加热块状银靶产生的等离子体XUV光谱.计算了T_e分别为65eV,86eV和130eV时,AgXIX4s-4P,4P-4d,4d-4f7条谱线在不同电子密度时的强度.根据AgXIX4d~2D_(s/2~-)4f~2F_(r/2)和4P~2P_(3/2)-4d~2D_(s/2)两条谱线的强度比,推导了激光银等离子体电子密度.当入射激光功率密度W为6×10~(12)W/cm~2时,银等离子体电子密度N_e=1×10~(20)/cm~3. 关键词：     

Steady State of the Dusty Plasma in a dc Discharge

The steady state formed by the diffusion of plasma particles in an inhomogeneous dusty plasma is investigated theoretically and compared with our previous experimental results [Nucl.Fusion Plasma Phys.20(2000)180 (in Chinese);Phys.Plasmas 8(2001)1459].The negatively charged dust grains with an average charge number of the order of 10^5 on a single grain enhance the plasma inhomogeneity by decreasing the diffusion velocity,and can cause significant depletion of electrons.The theoretical electron density profile is in good agreement with the experiment,and the theoretical profile of the electron-to-ion density ratio is in reasonable agreement with experimentally estimated data.     

The dielectronic recombination process in laser-produced Au plasmas

The calculations of the rate coefficients for dielectronic recombination (DR) along the NiI isoelectronic sequence in the ground state Au^{51+} through Cu-like 3d^9nln′f (n,n′=4,5,6) inner-shell excited configurations are performed using the spin-orbit-split array (SOSA) model. Resonant and nonresonant radiative stabilizing transitions and decays to autoionizing levels followed by radiative cascades are included. Collisional transitions following electron capture are neglected. The trend of the DR rate coefficients and the ratio of dielectronic satellite lines intensities with the change of the electron temperature are discussed.     

等离子体浸没注入超低能注入掺杂研究

A plasma immersion ion implantation(PIII) system based on inductively coupled plasma(ICP) technology was designed. The PIII system had a cylindrical chamber, and a radio frequency(RF) power was used to sustain discharge and a pulsed voltage source was provided to bias the wafer. The RF power was coupled into chamber by a non-coplanar two-turn circular structure coil. A Langmuir probe was connected to the PIII system to diagnose the plasma parameters. The probe diagnosis indicated that plasma ion density of the system achieves 10¹⁷m^-3, the uniformity of the ion density along radial direction achieves 3.53%. Boron (B) and phosphorus (P) doping experiments were performed on the system. Results from second ion mass spectrum (SIMS) tests showed that the measured injection depth is about 10nm and the shallowest is 8.6 nm (at 10¹⁸cm^-3), the peak ion concentration is below the surface of the wafer, and the ion dose reaches above10¹⁵cm^-2 and the abrupt 2.5 nm/decade.     

PLASMA IMMERSION ION IMPLANTER FOR THE MODIFICATION OF INDUSTRIAL AEROSPACE COMPONENTS

1　IntroductionPlasmaimmersionionimplantation (PIII) ,initiallydevelopedbyConradetalin 1 987,hase mergedasaviablealternativetoconventionalbeam lineionimplantationformetallurgicalappli cationsduetoitsconformalimplantationcapabili ty ,highthroughput,andcost effectiveness[1～ 6] .Asaresult,muchprogresshasbeenmadeinPIIIhardwareandunderstandingofplasmaphysicsper tainingtoindustrialapplications[7～ 10 ] .Inspiteofpromisingresults,thethintreatedlayer,complex ityofthePIIIprocess ,anddifficultyofi…     

Numerical investigation of non-local electron transport in laser-produced plasmas

Non-local electron transport in laser-produced plasmas under inertial confinement fusion (ICF) conditions is studied based on Fokker-Planck (FP) and hydrodynamic simulations. A comparison between the classical Spitzer--H\"arm (SH) transport model and non-local transport models has been made. The result shows that among those non-local models the Epperlein and Short (ES) model of heat flux is in reasonable agreement with the FP simulation in overdense region. However, the non-local models are invalid in the hot underdense plasmas. Hydrodynamic simulation is performed with the flux limiting model and the non-local model, separately. The simulation results show that in the underdense region of the laser-produced plasmas the temperature given by the flux limiting model is significantly higher than that given with the non-local model.     

中国ITER氦冷固态实验包层模块电磁安全分析

在中国ITER固态增殖实验包层模块(CH HCSB-TBM)的最新优化设计基础上,应用ANSYS参数化设计语言编程方法,对ITER实验包层模块(TBM)的电磁安全特性进行了计算分析.计算结果表明:HCSB-TBM最新优化结构设计的电磁安全特性符合设计要求.     

Theory of electromagnetic wave propagation in a plasma-filled corrugate waveguide immersed in a finite magnetized field

The linear theory of electromagnetic radiation from a high-power backward-wave-oscillator (BWO), travelling-wave-tube (TWT) with plasma-filled, sinusoidally corrugate waveguide driven by an intense relativistic electron beam (IREB) has been derived and analysed numerically. A general dispersion relation is presented for analysing a plasmafilled corrugate waveguide immersed in magnetized plasma in this paper. It is shown that the linear theory developed here is in good agreement with the previous work.     

Molecular Nitrogen Vibrational Temperature in an Inductively Coupled Plasma

Using a technique applied previously to vibrationally excited molecular nitrogen (N2^*) in the region of daytime and nighttime aurora,the emission intensity of the N2 second positive band system in an inductively coupled plasma (ICP) has been analysed and the vibrational temperature of nitrogen molecules in the ICP is thus determined.The result shows that the vibrational temperature increases with the increase of the neutral gas pressure from 0.04Pa to 10Pa,then decreases with the further increase of the pressure from 10Pa to 100Pa.Also,this is explained by using the Boltzmann relation between the vibrational temperature and the concentration of the vibrationally excited N2^*(X^1Σg^ ) molecules.     

激光诱导铝等离子体中原子和离子组分膨胀特性

为了了解等离子体中原子与离子组分的膨胀特性及背景气体存在状态下其运动状态的改变规律,设计了一系列实验,并进行了深入探究.采用波长为532 nm的纳秒激光剥蚀铝样品形成等离子体,并使用配有em ICCD检测器的C-T型三光栅单色仪对等离子体进行时序采集,同时使用2400 g·mm~(-1)的光栅替代窄带滤光片进行不同组分成像诊断,得到铝等离子体中Al Ⅰ (396.1 nm), Al Ⅱ (466.3 nm), Al Ⅲ (447.9 nm)的光谱分辨图像.在不同背景气压下采集了等离子体各组分光谱图像,探究背景气体对等离子体演化的影响.结果表明,在等离子体形成过程中,离子组分相对于原子组分分布在羽流前端,且角度分布较小.原子与离子组分的真空膨胀速度均处于10~4m·s~(-1)量级.等离子体中离子组分的运动速度较高,且其运动速度随着离子价态的增加而增大,但在本实验使用的能量密度范围下,随激光能量的变化波动不大.中性原子的运动速度较慢,但随能量的增加而增大.随着膨胀过程的进行,各组分羽流沿样品表面法线方向推进且发射强度逐渐降低,对应的羽流密度和温度也相应降低.环境气压逐渐增大时,各研究组分运动状态与在高真空度下时有明显区别.在气压大于1 Pa后,等离子体与环境气体发生相互渗透,膨胀前端出现的晕影,产生扰动,发生束缚缓速.且等离子羽因气压增大而收缩、与背景气体的碰撞概率增加,使得羽流发射强度加强,等离子体的寿命随之延长.提出的新颖诊断方法与实验所得结果可为等离子体组分动力学过程的研究提供参考.     

TeI4掺杂量对n型Bi2Te3基烧结材料热电性能的影响

采用区熔法结合放电等离子体快速烧结(SPS)技术制备了n型Bi2Te3基热电材料.在300-500K的温度范围内测量了各热电性能参数,包括电导率(σ)、塞贝克系数(α)和热导率(κ),研究了掺杂剂TeI4的含量(质量百分比分别为0,0.05,0.08,0.10,0.13和0.15wt%)对热电性能的影响.结果表明:试样的载流子浓度(n)随TeI4含量增加而增大,使电导率增大、塞贝克系数的绝对值先增大而后减小,从而导致品质因子(α2σ)呈先增加后降低的变化趋势;同时,由于异质离子(I-)以及载流子对声子的散射作用增强,可显著降低其晶格热导率.烧结材料的性能优值(ZT=α2σT/κ)对应于TeI4含量为0.08wt%有其最大值,约为0.92.此外,烧结材料的抗弯强度增加至80MPa左右,从而可以显著改善材料的可加工性以及元器件的使用可靠性.     

等离子体屏蔽效应对Ar~(16+)基态和激发态能级的影响

基于Rayleigh-Ritz变分原理,发展了一套处理弱耦合等离子体环境中多电子原子(离子)非相对论能量及其相对论修正的解析方法.通过考虑电子间交换相互作用以及内外壳层电子的屏蔽效应,计算了Ar~(16+)基态1s~2~1S、单激发态1sns~(1,3)S (n=2—5), 1snp~(1,3)P (n=2—5)和双激发态2snp~1P (n=2—5)非相对论能量及其相对论修正值(包括质量修正、单体和双体达尔文修正以及自旋-自旋接触相互作用项),讨论了等离子体屏蔽效应对能级的影响.结果表明:相对论质量修正和第一类达尔文修正占主导,比其他相对论修正项高出三个数量级.此外,等离子体屏蔽效应具有明显的态选择性,屏蔽效应对外壳层电子的影响大于内壳层电子,随着等离子体屏蔽参数的增加,外壳层电子轨道向外延展,激发态越高,延展程度越大.     

等离子体波背景下的光子Berry相位

利用光学度规将强激光脉冲激发的电子等离子体波描述为有效几何背景.借助于广义相对论中弯曲时空下的Maxwell方程组得到了探针光子在等离子体中电子等离子体波背景下(被处理为有效度规)所满足的运动方程及光子的Hamilton表达式.导出了电子等离子体波对光子Berry相位贡献的解析表达式并且对光子在真空中Berry相位的修正做了数值估算. 关键词： 电子等离子体波 等离子体 Berry相位     

A Pseudo Detailed Term Accounting Method for Radiative Opacity of Laser—Produced Plasmas

A statistical method is introduced to deal with the two-electron energies of a configuration in the detailed term accounting (DTA) approximation for the spectral line absorption in the radiative opacity of laser-produced plasmas in local thermodynamics equilibrium.The relativistic Hartree-Fock-Slater self-consistent field average atom model is used to select the reference ion with most probability and providing basically atomic data.In this way,fully frequency-dependent and spectral resolved opacity for heavy elements can be obtained readily for the primary design of radiation transfer in the inertial confinement fusion simulation.Opacities of Au plasmas are given.     

双波长输出He—Ne激光器测量氦等离子体中电子密度时空分布

用3.39μm和0.63μm同时振荡的双波长He-Ne激光器,首次测量了脉冲氦等离子体中电子密度(10~(14)～10~(15)cm~(-3)的时间和径向空间分布.     

Luminescence Properties of Ca4GdO（BO3）3：RE （RE=Eu^3＋,Tb^3＋） under VUV Excitation

We experimentally investigated the VUV excitation luminescence properties of Ca4 GdO(B03)3 :RE (RE=Eu^3 , Tb^3 )Ca4GdO(BO3)3:Eu3 and Ca4GdO(BO3)3:Tb^3 emitted bright red and green colour light, respectively, under 172 nm excitation, resulting from the favorable position of the host absorption band (186 nm) and efficient energy transfer from Gd^3 to activators (e.g. Eu^3 or Tb^3 ) by means of secondary absorption in the Ca4GdO(BO3)3 matrix. The f-d transitions of Eu^3 and Tb^3 in the host lattice are depicted.     

Cylindrical and spherical Gardner solitons and double layers in a dusty electronegative non-thermal plasma with two-temperature electrons

A precise theoretical investigation has been made on the cylindrical and spherical (nonplanar) Gardner solitons (GSs) and double layers (DLs) in a dusty electronegative plasma (composed of inertial positive and negative ions, Maxwellian cold electrons, non-thermal hot electrons, and negatively charged static dust). The reductive perturbation method has been used in derivation of the modified Gardner (MG) equation describing the nonlinear propagation of the dust ion-acoustic (DIA) waves. The MG equation admits solitary waves (SWs) and DLs solutions for σ around its critical value σ c (where σc is the value of σ corresponding to the vanishing of the nonlinear coefficient of the Korteweg de-Vries (K-dV) equation). The nonplanar SWs and DLs solutions are numerically analyzed and the parametric regimes for the existence of the positive as well as negative SWs and negative DLs are obtained. The basic features of nonplanar DIA SWs and DLs, which are found to be different from planar ones, are also identified. The implications of our results to different space and laboratory dusty plasma situations, are discussed.     

基于范阿伦卫星观测的槽区嘶声波冷等离子体色散关系的适用性评估

等离子体层嘶声波对电子的散射损失是地球内外辐射带之间的槽区(1.8≤L≤3)形成的主要机制.冷等离子体色散关系被广泛地运用于量化嘶声波对高能电子的散射效应研究中,而在真实的磁层环境中,热等离子体的存在会修正嘶声波的色散特性.基于范阿伦双星的观测数据,对比了利用磁场观测数据得到的槽区嘶声波观测幅值和反演幅值,并研究了空间位置与地磁活动水平对嘶声波冷等离子体色散关系适用性的影响.结果表明,冷等离子体近似整体上高估了嘶声波的幅值,观测幅值与反演幅值的差异有着很强的日夜不对称性,而没有明显的地磁活动强度依赖性.此外发现,波动磁场的反演强度在低频(高频)处显著低于(高于)观测强度,意味着冷等离子体近似整体上高估(低估)了嘶声波对槽区较低(较高)能量电子的散射强度.研究证明,槽区嘶声波冷等离子体色散关系的适用范围有很强的空间区域与频率局限性,这对深入理解槽区电子的动态演化过程有非常重要的意义.     

ICP-AES/ICP-MS测定胡芦巴不同部位矿质元素

采用电感耦合等离子体-原子发射光谱法(ICP-AES)和电感耦合等离子体-质谱法(ICP-MS)联合测定胡芦巴叶、茎和种子中13种矿质元素的含量,并考察了13种元素在胡芦巴不同部位的分布情况.分析结果表明,胡芦巴中13种矿质元素在各部位中的加合量(μg·g-1)由高到低的顺序依次为:叶(527644.60)＞茎(382441.80)＞种子(108389.20),各元素在不同部位分布也不同,其中Ca、K、Mg、Mn、Zn、Se在叶中含量总体相对较高;而P、Cu、Cr在种子中含量较高,其他各元素在3个部位的含量差异不大.此外,种子中Zn/Cu仅为5.30,有利于调节人体中胆固醇的异常代谢,与胡芦巴降血脂活性部位在种子中的结果一致.     

HL—1装置等离子体品质进展

本文概述HL-1装置等离子体品质参数空间在1985—1988年的进展及其与装置各项技术改造措施和等离子体基本参数(因素)之间的内在联系.