用于激光等离子体诊断实验的二倍频探针光系统

为了满足基准物理实验的要求,准确地探测出靶面的等离子体的电子温度、密度、电子离子漂移速度等参数,在星光Ⅱ激光装置上发展了一束二倍频激光作为探针光。通过模拟实验已经证实了该探针光的二倍频总能量大于5J,焦斑尺寸小于100μm,可以满足激光与等离子体相互作用的高功率要求。目前,该探针光系统已经用于用于激光等离子体诊断实验的常规运行。     

用于等离子体诊断的ps激光探针

 ps激光探针作为激光等离子体诊断的探针光源，它是通过两次倍频和两次受激喇曼散射，将波长为1 054nm、脉宽约为1ns激光转换成波长为308nm、脉宽小于30ps的紫外光。研究结果表明：探针光系统输出能量大于1mJ，脉宽小于30ps，均匀性较好，运行成功率大于90%，满足了激光等离子体诊断的要求。     

X光激光实验中的等离子体状态诊断

在LF-12激光装置上,将500～600J、约1.5ns脉冲宽度的Nd玻璃激光聚焦成约120μm宽、20mm长的线作用到1mm厚的锗平面靶上。在靶室内设置具有空间分辨本领的平晶谱仪(测量波长范围在0.6～0.9nm)诊断锗等离子体状态。用2p-nd(n≥4)能级跃迁的类Ne离子谱线间的相对强度比估计等离子体电子温度在400～600eV。在实验中测到的线谱主要是类Ne GeXXⅢ离子产生的,类F GeXXⅣ离子产生的谱线次之,类Na GeXXⅡ离子产生的谱线比较弱。并且初步观察到线状等离子体轴向分布均匀性和横向离子分布特征。     

三倍频激光等离子体X射线转换研究

利用“星光Ⅱ”高功率激光装置三倍频激光（波长０.３５μｍ,能量５—９０Ｊ,焦斑直径约２００μｍ,脉冲宽度４００—８００ｐｓ）辐照多种材料（Ｃ,Ａｌ,Ｃｕ,Ａｕ）靶,对于不同激光功率密度,研究软Ｘ射线转换和发射能谱．结合０.３５μｍ激光辐照Ａｌ靶的质量烧蚀率和等离子体喷射速度与激光功率密度的定标关系进行数值模拟,对于激光功率在１０^１３—１０^１５Ｗ／ｃｍ²理论模拟结果与实验结果符合得很好 关键词：     

激光等离子体2660紫外探针及干涉系统

成功地在六路高功率Nd玻璃激光装置上建立了2660紫外激光探针和适合紫外波段的Normaski干涉仪,首次将可见波长的连续激光应用于紫外干涉仪中靶成像调整和光路准直。利用该紫外光干涉仪,在铜柱状靶(φ500μm)上测量了厚等离子体中高达0.6n。的电子密度。     

激光等离子体探针及应用研究

本文介绍用阴影、纹影相干涉方法确定等离子体折射系数变化的原理。分析了等离子体中的非线性效应和对光探测系统的基本要求。并简要叙述了实验上采用的后向喇曼探测束,给出了等离子体干涉、纹影和阴影的测量结果。     

软X射线激光探针诊断高Z材料等离子体

激光辐照靶产生的等离子体电子密度的诊断对于惯性约束聚变、高能量密度物理等相关领域的研究具有重要意义,特别是高Z材料等离子体临界面附近的电子密度分布信息的测量.利用软X射线激光作为探针是诊断等离子体电子密度分布的一种重要方法,但在诊断激光辐照高Z材料产生的等离子体研究中,遇到了高Z材料等离子体自发辐射过大的问题,难以开展.为此,针对软X射线激光的特点,发展了多种具体的实验技术.通过综合利用这些技术,大大的抑制了待测等离子体自发辐射对信号的影响,使得软X射线激光探针诊断高Z材料等离子体成为可能.作为典型例子,实验诊断了激光辐照金平面靶的等离子体,获得了清晰的实验图像,表明相关的技术是有效和可行的.     

用于Z-pinch诊断的266nm激光探针分幅阴影成像系统

采用Nd-YAG激光器的四倍频激光(266nm)设计了激光探针分幅阴影成像系统，该系统具有时间分辨率和收光效率高，测量范围大，可有效屏蔽可见光干扰的优点，在钨丝阵实验中成功获得晚期内爆等离子体的分布图像.对系统结构和性能参数做了介绍，对测量结果进行了讨论. 关键词： Z-pinch 激光探针 等离子体分布 分幅成像     

用于激光等离子体诊断的硬X光能谱仪

介绍了利用滤片和探测器阵列组合的硬X光能谱仪(简称FFS)的工作原理,结构性能和数据处理。文章最后给出了FFS在惯性约束聚变(ICF)实验中测到的硬X光谱的典型结果。     

用于等离子体电位测量的电容探针和发射探针

本文给出了发射探针和电容探针测量等离子体电位的实验和方法。发射探针采用直流功率加热，并在较强电子发射条件下运行（Ｉ_（ｅ０）／Ｉ_（ｅ０）＞１）。电容探针表面二次电子发射系数δ≥１。本文对发射探针的电子发射性能、工作电流、电容探针的输入、输出电压关系进行了标定实验。得到了电容探针的校准系数分别为３×１０（－３）、５×１０（－４）。实验给出了ＭＭ－４会切中心等离子体电位Ｖ_（ｐ４）＝－８２±９－１２２±１２Ｖ；ＭＭ－４Ｕ东、西会切中心等离子体电位分别为Ｖ_（Ｐ４ｕ１）＝－５２．９±３．２Ｖ，Ｖ_（Ｐ４ｕ２）＝－６２±３．２Ｖ。     

正态分布随机数发生器及其在模拟光传输软件中的应用

利用计算机高级语言提供的伪随机数发生器,通过“高斯筛选”和“求平均值”两种方法,开发出满足正态分布的随机数发生器。将其应用于分析大型激光装置光路稳定性的模拟软件中,成功地完成了对“神光Ⅲ原型装置四程放大器”的光路稳定性分析。     

A multiple laser beam probe system for turbulence diagnostics

Deatils are given of a multiple laser beam probe for sizing and velocity measurements in turbulent media. Sample results are presented in the case of thermal turbulent convection in a model buble chamber.     

飞秒脉冲的二次谐波理论和实验研究

本文分析了小信号情况下飞秒脉冲的倍频特性,在非耗尽近似下,得出了飞秒脉冲二次谐波波形及效率的解析解,在时间域内,对一般条件的耦合波方程进行了数值解,分析了相位失配对飞秒脉冲倍频波形及效率的影响。 用0.5mm厚的一类匹配LBO晶体对碰撞锁模激光器产生的80fs超短脉冲进行了腔外倍频实验,实验结果与理论计算符合得很好。     

Second harmonic generation in plasma in the presence of SBS

The mechanism of second harmonic generation in the presence of intense-radiation SBS in plasma is considered under the condition that the incident beam has no time for filamentation. The mechanism is based on the formation of low-frequency plasma-density perturbations that are optimal for this effect in the field of scattered waves. The theoretical calculations are compared with the experimental data.     

Second harmonic generation of a self-focused Hermite-Gaussian laser in plasma

Second harmonic generation (SHG) using intense Hermite-Gaussian laser beam (HGLB) propagating through the plasma for mode-indices m = 0 and m = 1 is reported in the present work. Ponderomotive force induced density perturbation beats with the oscillatory velocity of electrons at incident laser frequency, generate the second harmonic nonlinear current that give rise to SHG. Using paraxial approximations, we have derived the coupled equations for the beam width parameter of HGLB and second harmonic's normalized amplitude. Resonance condition is obtained by considering wiggler magnetic field which providing an extra momentum to the second harmonic photon and this result a significant increase in the amplitude of SHG. Our analysis shows the prominent rise in normalized amplitude of second harmonic on increasing the value of the intensity of fundamental laser pulse, normalized wiggler magnetic field and normalized density of plasma. It is notified that the gain of SHG is more prominent for m = 1. Dependency of laser and plasma parameters on SHG is also reported in the current work.     

Second harmonic generation accompanying linear mode conversion in a laser-produced plasma

Second harmonic (SH) generation in a laser produced plasma (NdYAG laser with wavelength 1.06 μm, pulse duration 30 ps, intensity 10¹³Wcm^-2) was investigated experimentally as a function of polarization and angle of incidence of the laser beam. The results are in agreement with theoretical predictions for SH generation in the presence of linear mode conversion in the plasma.     

Advanced high-pressure plasma diagnostics with hairpin resonator probe surrounded by film and sheath

The hairpin probe using microwave resonance in plasma is applicable to high pressure 1.33×10 3-1.01×10 5 Pa)) as developed recently.In this work,an analytic model of the hairpin resonator probe surrounded by a thin dielectric layer and a sheath layer is proposed.The correction factor due to these surroundings is analytically found and confirmed by electromagnetic field finite difference time domain simulation,thus enabling the accurate measurement of electron density in a high-pressure non-equilibrium uniform discharge.     

Second harmonic generation of high power Cosh-Gaussian beam in cold collisionless plasma

The purpose of this study is to explore the second harmonic generation (SHG) of a high power Cosh-Gaussian beam in cold collisionless plasma. The ponderomotive force causes carrier redistribution from high field to low field region in presence of a Cosh-Gaussian beam thereby producing density gradients in the transverse direction. The density gradients so produced the results in electron plasma wave (EPW) generation at the frequency of the input beam. The EPW interacts with the input beam resulting in the production of 2nd harmonics. WKB and paraxial approximations are employed for obtaining the 2nd order differential equation describing the behavior of the beam's spot size against normalized distance. The impact of well-established laser-plasma parameters on the behavior of the beam's spot size and SHG yield are also analyzed. The focusing behavior of the beam and SHG yield is enhanced with an increase in the density of plasma, the radius of the beam and the decentred parameter, and with a decrease in the intensity of the beam. The results of the current problem are really helpful for complete information of laser-plasma interaction physics.     

Second harmonic conical refraction

Second harmonic intensity patterns generated in α-iodic acid have been observed. Free and forced conical patterns occur, when the fundamental wave vector lies along a second harmonic or fundamental optic axis, respectively.