CO2激光打靶中的高次谐波发射

本文在文献[1]的基础上,进一步计算了高次谐波的场结构与转换率。计算中,通过假设等离子体密度的双线性分布而考虑了临界密度面附近的密度轮廓变陡效应。所得解析结果能较为满意地解释CO₂激光打靶实验中已观察到的有关高次谐波发射的物理现象。 关键词：     

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：     

CO_2激光打靶中的高次谐波发射

本文在文献[1]的基础上,进一步计算了高次谐波的场结构与转换率。计算中,通过假设等离子体密度的双线性分布而考虑了临界密度面附近的密度轮廓变陡效应。所得解析结果能较为满意地解释CO_2激光打靶实验中已观察到的有关高次谐波发射的物理现象。     

飞秒强激光与欠稠密等离子体相互作用中的二次谐波辐射

对超短超强激光脉冲 (45fs,6× 10 17W /cm2 )与光致电离氦气形成的欠稠密等离子体相互作用中的二次谐波辐射进行了实验研究。测量了多种打靶强度的飞秒激光脉冲与不同气体密度氦气相互作用的二次谐波光谱 ,得到在欠稠密等离子体中二次谐波辐射与打靶激光能量的关系 ,分析了产生二次谐波辐射产生的物理机制 ,在考虑了强短脉冲激光电离气体产生的等离子体径向电子密度梯度因素 ,基于非线性作用过程的理论预期曲线与实验结果较好地吻合     

三温与多温电子等离子体的自由膨胀与快离子的产生

本文介绍三温与多温电子等离子体自由膨胀的理论模型。自相似解成功地再现了在激光等离子体自由膨胀中离子速度分布呈现的三峰和多峰结构,这些结构已在激光打靶的实验中频繁地观察到。计算结果表明:快离子谱峰值的数目与构成等离子体的电子分量的数目密切相关;相邻两峰之间坑的深度对相应电子温度的比值非常敏感;坑的位置依赖于相应电子数密度的比值,它们也受其它电子分量耦合的影响。最后还讨论了自相似解的适用范围。 关键词：     

超短超强激光与气体靶相互作用中的背向受激Raman散射

 实验诊断测量了超短超强激光与气体靶相互作用产生的背向受激Raman散射,在实验条件下呈现强耦合模式,背向受激Raman散射出现非线性Stokes多峰伴线结构,峰值的频率间隔小于等离子体波的频率,可以大致地推断出激光打靶过程中产生的等离子体密度偏低,其结果与等离子体强耦合理论计算结果一致。     

激光干涉技术在超声速气体喷嘴特性研究中的应用

在激光与物质相互作用的实验中,气体靶通常由超声速喷嘴在高背压下向真空中高速喷射气体产生。激光与气体靶相互作用时确定打靶条件对整个实验有着十分重要的意义。为了得到不同实验条件下气体靶密度的分布特性，采用马赫-曾德尔干涉法测量了气体靶密度分布，获取了干涉图样。使用基于傅里叶变换的条纹处理方法测得的干涉图样，得到不同实验条件下气体分子密度的全空间分布。实验表明：用M-Z干涉仪测量超声速气体喷嘴产生的气体靶密度分布十分有效。基于傅里叶变换的条纹处理方法具有精度高、实时性好的优点，为打靶时气体靶密度的实时测量提供了可能。     

1.053μm激光打靶产生的二次谐波

测量了基频激光打靶条件下不同角度的二次谐波光谱,得到了谐波光强随发射角度的变化关系以及能量转换效率随激光强度变化的曲线.实验现象可能与参量衰变级联造成的Langmuir湍流有关 关键词： 二次谐波发射 激光等离子体 共振吸收 离子声衰变不稳定性     

双示踪元素X射线能谱诊断激光等离子体电子温度

在“星光Ⅱ”激光装置上对Mg/Al混合材料平面靶和Mg/Al示踪层金盘靶进行三倍频激光打靶实验,用平面晶体谱仪测量靶材料发射的X射线能谱,获取了示踪离子谱线实验数据.采用多组态Dirac-Fock方法计算所需原子参数,并在局域热动平衡条件下建立了双示踪离子谱线强度比随电子温度变化关系.在此基础上由双示踪元素等电子谱线法确定了Mg/Al混合材料平面靶及金盘靶激光等离子体的电子温度 关键词： 电子温度 激光等离子体 X射线能谱     

激光照射中Z薄靶等离子体状态的计算-激光等离子体相互作用的理论模拟(Ⅰ)

本文叙述用一维非平衡辐射流体力学激光打靶程序模拟计算高功率密度(~10¹³W/cm²)激光照射中Z介质薄靶形成的等离子体状态。考虑的物理过程有轫致、光电离、电子碰撞电离及它们的逆过程,Compton散射过程等。Compton散射采用Fokker-Planck近似;电子和离子热传导采用限流扩散近拟;光子方程采用多群限流扩散近似;用平均原子模型计算布居数。激光的吸收主要考虑逆轫致吸收。用功率密度分别为5×10¹³W/cm²和1×10¹⁴W/cm²,波长0.53μm,脉宽450ps的激光从两面和单面打se薄靶,模拟计算结果与国外的实验结果^[1]一致。     

KTN薄膜脉冲激光沉积过程的机理研究

根据能量平衡原理,导出了脉冲激光作用靶材的烧蚀率公式,并根据流体动力学理论,得出了脉冲激光产生的等离子体的空间运动特性方程,将靶材烧蚀率公式与等离子体空间动力学方程结合起来,根据实验研究了不同激光功率密度和波长对Kta_0.65Nb_0.35O₃(KTN)薄膜沉积特性的影响,得到了一些有价值的结果,并对结果进行了详细的讨论,理论计算结果与实验大体符合. 关键词： PLD技术 烧蚀率 等离子体 KTN薄膜     

Laser effects on the donor states in V-shaped and inverse V-shaped quantum wells

Laser effects on the electronic states in GaAs/ Ga_1−xAl_xAs V-shaped and inverse V-shaped quantum wells under a static electric field are studied using the transfer matrix method. The dependence of the donor binding energy on the laser field strength and the density of states associated with the impurity is also calculated. It is demonstrated that in inverse V-shaped quantum wells under electric fields, with an asymmetric distribution of the electron density, the position of the binding energy maximum versus the impurity location in the structure can be adjusted by the intensity of the laser field. This effect could be used to tune the electronic levels in quantum wells operating under electric and laser fields without modifying the physical size of the structures.     

High-order harmonic generation and multi-photon ionization of Na2 in laser fields

In this paper high-order harmonic generation （HHG） spectra and the ionization probabilities of various charge states of small cluster Na2 in the multiphoton regimes are calculated by using time-dependent local density approximation （TDLDA） for one-colour （1064 nm） and two-colour （1064 nm and 532 nm） ultrashort （25 fs） laser pulses. HHG spectra of Na2 have not the large extent of plateaus due to pronounced collective effects of electron dynamics. In addition, the two-colour laser field can result in the breaking of the symmetry and generation of the even order harmonic such as the second order harmonic. The results of ionization probabilities show that a two-colour laser field can increase the ionization probability of higher charge state.     

Threshold dependence of the vibrational excitation of molecules on laser radiation intensity

The collisionless vibrational excitation of a polyatomic molecule in an IR laser radiation field has been theoretically studied. It has been shown that (i) the degree of vibrational excitation (namely, number 0000 of vibrational quanta of a molecular mode near-resonant with the IR laser field that are absorbed by the molecule) is low if laser pulse intensity P (energy flux density in the laser beam) is lower than a certain critical value P _cr; (ii) the degree of excitation abruptly increases after crossing the boundary where P = P _cr; (iii) this effect is attributed to two properties inherent in polyatomic molecules, namely, the anharmonicity of the vibrational mode interacting with the laser field and the energy exchange with other modes; and (iv) at P > P _cr, number 00000 is determined only by energy density Φ = Pτ_P, where τ_P is the laser pulse duration, 00000 monotonically increases with increasing Φ. The model is in good agreement with the experimental data.     

Varied laser induced damage phenomena of gold coated gratings for pulse compression

In this paper, gold-coated gratings for pulse compression have been prepared and their laser damage experiments have been performed. Varied laser damage morphologies have been observed: when a 60 fs-pulsed laser with energy density slightly higher than the damage threshold was used, damage morphology with a characteristic of discrete distribution of small pits was appeared. These damage pits are linearly distributed at the junction of ridges and grooves. If the laser energy density is much higher than the damage threshold, the gold films was overall ablated and the grating structure disappeared. Besides, if the gold film has poor adhesion, it was peeled off. When a 450 ps-pulsed laser with energy density slightly higher than the damage threshold was used, part of grating ridges will be ablated and an obvious line exists between the ablated area and the unchanged area. In theory, the laser induced temperature field and stress field in gold-coated gratings were calculated based on the electromagnetic field using the finite element method. It is demonstrated that the temperature and thermal stress distribution characteristics are affected by the laser heating rate and the heat diffusion time (the calculated diffusion time ranges from 6 fs to 450 ps), which determines the laser damage characteristics. The possible damage drivers have electron hydrodynamic pressure, thermal ablation and thermal stress.     

共振吸收的场结构与密度轮廓变陡

本文采用一种新的解析方法,讨论了激光等离子体中的共振吸收场结构与密度轮廓变陡的问题,得到了共振吸收场结构的解析表达式,由此推导得出的以初等函数表示的共振吸收系数,能在所有入射角的范围内都与计算机数值解相符合。另外,有关稳态密度轮廓变陡的解析计算,也正确地反映了有关实验及计算机模拟的结果。 关键词：     

Spectroscopy and laser operation of Nd-doped mixed sesquioxides (Lu1?x Sc x )2O3

We report on crystal growth, spectroscopic investigations, crystal field tuning, and laser experiments of neodymium doped mixed sesquioxides (Lu_1?x Sc _x )₂O₃. Crystals were grown by the Nacken?CKyropoulos and the Heat-Exchanger method. Emission spectra for several mixing ratios are presented. Cw laser experiments were carried out with a 0.35?at.%-doped Nd:Lu_1.82Sc_0.18O₃ crystal by using a Ti:sapphire laser as pump source, achieving a maximum slope efficiency of 47?% with respect to the absorbed pump power and a maximum output power of 356?mW at a wavelength of 952.7?nm. To the best of our knowledge, this represents the first continous wave (cw) laser operation of a Nd-doped mixed sesquioxide.     

Theoretical study of multi-mode optically pumped NH3 FIR laser

The two or multi-mode optically pumped NH₃ FIR laser had been studied theoretically. The NH₃ molecular gas was assumed to be a three-level system and obeyed the time-dependent behavior of the density matrix equations. Considering the situation of playing the two or multi-mode optical pumping and the FIR laser field were same polarized. The gain coefficient and the output FIR power of the system could be calculated by using the iteration method.It had been predicted that the two or multiple longitudinal mode optically pumped NH₃ FIR laser could have a greater output power or higher lasing efficiency than single mode pumped FIR laser under suitable selected operating parameters of laser.Supported by The Education Foundation of PRC.     

Nonlinear absorption of CO2 laser radiation by nonequilibrium carriers in germanium

Nonlinear absorption of CO₂ laser pulses at the multi-MW level has been studied in n-type germanium at room temperature. This nonlinear absorption limits the level of CO₂ laser intensity that can be transmitted through an optical grade germanium crystal. The observed nonlinearity may be interpreted in terms of nonequilibrium electron-hole pairs generated by hot electrons created by the intense laser field. The number of nonequilibrium carriers generated is measured by photoconductivity experiments, and the results are correlated to the absorption measurements.     

Synthesis and characterization of LaB6 thin films on tungsten, rhenium, silicon and other substrates and their investigations as?field emitters

The paper deals with the comparative study of nanocrystalline Lanthanum hexaboride (LaB₆) thin films grown on various substrates by Pulsed laser deposition and Arc plasma method. Field emission studies were carried out on LaB₆ films deposited on various substrates show metallic behavior of the emitters. The high value of field enhancement factors, indicating that the electron emission from LaB₆ nanoscale protrusions deposited on emitter surface. The post field emission surface morphology of the emitters showed no significant erosion of the films during continuous operation. The observed behavior indicates that it is linked with the growth of LaB₆ films on substrate crystal structure. The LaB₆ nanocrystallites/nanowires films were synthesized using arc plasma method shows good emission current stability. The LaB₆ micro/nanocrystallites were also obtained by picosecond laser irradiation which gives high enhancement β factor, and good emission current stability along with high current density. The results reveal that nanocrystalline LaB₆ films, exhibit high resistance to ion bombardment and excellent structural stability and are more promising emitters for practical applications in field emission based new generation devices.