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。     

“PPAS” X-RAY ABSORPTION SPECTROSCOPY IN LASER-PRODUCED ALUMINUM PLASMA

We have developed and successfully demonstrated the "point projection absorption spectroscopy (hereafter abbreviated to PPAS)" technique to record keV X-ray absorption spectra in the coronal region of laser produced aluminum plasma which provides spatial information in the corona. Absorption spectrum of the Al Ⅻ 1s²-1s2p resonant line for time delays up to 250, 500 and 750 ps after the peak of the incident laser pulse have been observed. Analysis of an absorption spectrum should allow a high spatial resolution (< 25μm) history of the absorbing ion population density to be determined. The 1-D hydro-code JB19 has been used to simulate the experiment and the predictions are compared to the observations. Such comparison can be useful in validating parts of the codes used for gain prediction on recombination X-ray laser transitions.     

基于奇异值分解的数字波前拟合算法

提出了基于奇异值分解、采用泽尼克多项式拟合干涉波前的算法,该算法直接从线性方程组入手,对矩阵进行奇异值分解分解,在求解逆矩阵的过程中,采用阈值法对奇异值的倒数进行非常规的置换(∞→0),可直接得到系数向量。理论分析和实验证明,相对于传统的格拉姆施密特正交法,该算法可首先通过求解条件数判断线性方程矩阵是否奇异,对于解决病态方程组或奇异矩阵的最小二乘问题,有很好的稳定性,避免了由最小二乘构造的法方程组出现病态而引入的计算误差,且易于编程。     

基于“神光-Ⅱ”装置的飞秒拍瓦级光学参量啁啾脉冲放大的特性分析与系统设计

用计算机仿真分析了光学参量啁啾脉冲放大（OPCPA）的特性及其影响因素（如相位失配、高阶非线性效应等）-就脉冲放大机理、时间同步、光谱漂移、增益窄化等相似问题与现有的啁啾脉冲放大技术做了比较与讨论-基于“神光-Ⅱ”装置，设计了飞秒拍瓦级OPCPA系统，以期望实现快点火- 关键词： 超短超强激光 啁啾脉冲放大 光学参量啁啾脉冲放大 数值模拟     

软X射线激光偏折法测量激光等离子体电子密度分布

利用脉宽约为50ps的类镍银139nm软X射线激光作为探针,探测由脉宽80ps的驱动激光打C8H8靶产生的等离子体在1ns后的电子密度分布信息,获得了清晰的莫尔条纹图像.对结果的处理,给出了峰值电子密度为11×1021cm-3,并对在靶面附近莫尔条纹的消失现象作了初步解释 关键词： 软X射线激光探针 莫尔条纹 等离子体电子密度     

High power pulse amplification of ytterbium-doped double-clad fiber amplifier

By solving a set of time-dependent equations,the characteristics of the ytterbium-doped double-clad fiber amplifier are presented.Besides the steady state in the fiber of the upper-state population,pump power and amplified spontaneous emission without the input signal,the dynamic characteristics of the high power Gaussian pulse amplification like the evolution of pulse waveform distortion,upper-state population distribution and stored energy and pulse energy of the amplifier under the forward and backward pump, are simulated.The relations between the output pulse energy of the amplifier and the different input pulse peak power or pump power are also discussed.The models and results can provide important guide for the design and optimization of the high power pulse amplification.     

Single Mode Er-Doped π-Phase-Shifted Distributed Feedback Fibre Grating Laser

A novel method incorporating the shielded method and the post-processing method has been proposed to fabricate the π-phase-shifted fibre grating. Then an Er-doped π-phase-shifted distributed feedback fibre grating laser has been fabricated using the grating. The laser threshold is 20mW. When pumped with 90mW light at 980nm, the laser gives an output of 1.1mW. Its signal-to-noise ratio is better than 60dB. It is demonstrated that the laser is single mode operation by means of a Fabry--Perot scanning interferometer.     

激光频带宽度对二次谐波时空分辨结构的影响

本文报道用条纹相机在沿与激光光轴成90°方向拍摄的二次谐波发射的时空分辨结构,宽频带激光打靶与窄频带激光打靶表现出明显的差异,用孤立波产生理论进行分析,得出与实验基本相符的结果。 关键词：     

辅助光斑对10μm半径级小尺度自聚引发谐波辐射的作用

本文的最新实验表明,单个10μm半径级的激光斑在预形成的激光等离子体中不能有效激励90°侧向3ω₀/2谐波发射。但配合同样尺寸的辅助光斑,在满足一定位置和角度条件下却容易引发这种发射。使用双等离振子衰变理论,结合动态自聚细丝模型分析了这一现象的起因。     

利用皮秒脉冲激光驱动瞬态X射线激光

报道了利用皮秒激光驱动产生瞬态类镍银X射线激光的实验结果.采用一路脉冲宽度为数百皮秒的激光作为预脉冲，配合另一路皮秒激光作为主脉冲联合驱动平面靶，获得了一定强度的类镍银X射线激光输出，输出能量约为5—10nJ. 关键词： 瞬态X射线激光 长短脉冲联合驱动 皮秒脉冲激光