基于发射光谱的DF激光器光腔温度与粒子数分布

 建立了谱线增益系数与温度、粒子数分布之间及谱线增益系数与谱线强度之间的关系式,对一台燃烧驱动DF激光器的发射光谱进行了测量,利用发射光谱数据计算得到光腔温度为381.4 K,分布在振动态能级1与0,振动能级2与1,振动能级3与2的粒子数之比分别为0.60～0.62, 0.676 4, 0.71～0.74。     

Tm3+/Yb3+共掺碲铅锌镧玻璃的能量传递和上转换发光

制备了Tm3+/Yb3+共掺TeO2-PbO-ZnO-La2O3玻璃,研究了玻璃红外吸收光谱和980 nm激光抽运下上转换发光光谱,分析了上转换发光机制.基于Tm3+和Yb3+的能级图及上转换机制建立了速率方程,得出了稀土离子各能级的粒子数分布密度以及Tm3+与Yb3+之间的能量转移系数Cbi(i=0,1,3).结果表明,随着PbO加入,Yb3+:2F5/2与Tm3+:3H4间的能量转移不断增加,上转换蓝光的发光强度明显增强.     

环形腔PbSe量子点单模光纤激光的计算机数值模拟

在PbSe/UV胶量子点光纤环形腔激光器实验的基础上,通过建立并数值求解粒子数速率方程和光功率传播方程等,对1550nm的激光输出特性进行了数值模拟。计算的抽运阈值功率、单/多模激光输出功率随抽运功率的变化、合适的PbSe掺杂浓度、单模激光功率随输出耦合比的变化等,与实验结果基本吻合。通过对PbSe量子点光纤中激光功率分布的研究,给出了粒子数密度的反转条件:N2/N1≥0.45,该条件可由1550nm波长处粒子数反转的吸收截面与辐射截面之比得到。研究了掺杂浓度对激光功率的影响,给出了合适的掺杂浓度范围。     

双包层Er3+/Yb3+共掺光纤激光器动态特性的分析

分析了弛豫振荡前上能级Er³⁺、Yb³⁺粒子数的变化和弛豫振荡时Er³⁺上能级粒子数的变化情况以及弛豫振荡时激光功率的变化规律,结果表明:弛豫振荡时的激光峰值功率远大于稳态时的激光功率.     

在低价氮离子中实现3s-2p软X射线的最佳条件研究

从实现离子的基态和激发态之间粒子数反转的主要参量入手，数值计算了基态的 粒子数密度、上能级和下能级的统计权重之比、三体复合速率和自发辐射衰减速率之比等每个参量对反转粒子数密度的影响，并且以基于光场感生电离（OFI）复合机制B－likeN系统为例对实际系统进行分析讨论，给出了实现基于光场感生电离B-like N45.21nm3s-2p跃迁激光放大的最大激光功率密度。     

相移法测量寿命的理论分析

本文从理论上分析了利用调制的单模激光场共振激发来测量原子或分子的寿命.结果表明:感生荧光或共振荧光信号与调制信号间的相移主要来自三个过程:(1)由原子的横向弛豫时间及激光线宽决定的激发过程;(2)由激发能级及其他能级上粒子数衰减过程;(3)与系统达到平衡态粒子数分布所需的弛豫时间有关的碰撞激发过程.讨论了在不同的情况下它们的影响,并在分析中考虑了多普勒加宽的影响.     

3μm与2μm级联振荡Ho3+:ZBLAN光纤激光器的动态特性分析

基于传输速率方程,对Ho3+:ZBLAN光纤激光器的动态特性--上能级粒子数以及输出激光功率的弛豫振荡特性进行了数值分析.通过忽略光纤参数对传输方向的依赖性,抽运光和信号光的功率传输方程被分别简化处理.结果表明,在5I6能级的粒子数首先经历一次弛豫振荡后,5I6和5I7能级的粒子数交替弛豫振荡并达到稳态;同样,在3μm波长的激光功率首先经历一次弛豫振荡后,3μm和2μm波长的激光功率交替弛豫振荡并达到稳态,而且,弛豫振荡时的峰值功率远大于稳态时的激光功率.     

双包层Er-Yb共掺光纤放大器上能级粒子数分布研究

基于速率方程和功率传播方程, 数值分析了双包层Er-Yb共掺光纤放大器在波长为972nm的泵浦光作用下, 分别采用三种不同泵浦方式, 其Er3+和Yb3+上能级粒子数分布情况. 数值结果表明,Er3+上能级粒子数分布受信号功率影响作用大, 激发率基本保持在50％以上; Yb3+上能级粒子数分布受泵浦功率影响作用大, 激发率基本保持在10％以下, 该结论对双包层Er-Yb共掺光纤放大器的性能研究具有一定指导意义.     

二极管抽运铷蒸气激光的物理特性

结合激光微观动力学和热传学,充分考虑到发射激光时的各能级粒子数和热力学分布特性,建立了用于分析二极管抽运铷金属蒸气激光物理特性和增益腔内的温度分布模型,得到了抽运功率和激光输出、光-光转换效率及各物理参数之间的关系,分析了有效提高抽运能量吸收的具体措施,揭示了2P3/2和2P1/2两个精细能级之间的集居数弛豫对半导体抽运碱金属蒸气激光器(DPAL)物理特性的影响。结果表明:在设计不同用途DPAL时,必须要综合考虑各种因素,以确定相应的最佳结构参数。     

LD抽运腔内和频571.6nm连续波黄光激光器

报道了全固态连续波571.6nm黄光激光器.黄激光是分别由两片Nd∶YAG的1444nm和946nm谱线非线性和频产生,两条谱线在各自晶体对应能级跃迁分别为4F3/2-4I15/2和4F3/2-4I9/2.实验中采用复合腔结构,利用RTP晶体II类临界相位进行内腔和频,当注入到两片Nd∶YAG晶体的抽运功率分别为25W和14.8W时,获得562mW的连续波571.6nm黄激光输出,4h功率稳定度优于±2.9%.     

Eu:Fe:LiNbO3晶体非简并四波混频的研究

用波长为623.8nm的He-Ne激光作信号光和一束泵浦光,用波长为488.0nm的Ar⁺激光作另一束泵浦光,在Eu:Fe:LiNbO₃晶体中实现了非简并四波混频,获得了波长为488.0nm的变频相位共轭光,同时还产生了波长为632.8nm的同频相位共扼光。本文对上述实验结果进行了定性分析。     

ZnWO4∶Sm3+晶体光谱与上转换发光

采用Czochralski法生长出了ZnWO₄∶Sm³⁺单晶(Sm₂O₃=0.1wt%)，测量了晶体的吸收光谱.利用激光Raman谱仪在He-Ne激光器632.8nm波长激光激发下，观测到448，471，505，533nm的上转换锐线荧光，对其发光机理进行了探讨. 关键词：     

激光高反射膜的研究

研究混合膜（TiO2 Ta2O3;Ta2O5 ZrO2)的色散规律，用Ta2O5 ZrO2和SiO2成功地镀制出两个波段（632．8nm,1.06μm)的激光反射膜，使激光破坏阈值提高5％－15％（1．06μm)，膜层吸收小，机械强度增加。     

大视场反射式激光扩束系统光学设计

激光扫描捕获系统通过对激光光源进行扩束变换,压缩光源的发散角度,可减少在远距离传输中的能量损失。为满足某通信实验需要,设计一种放大倍率为10倍,光源扫描视场为4840的小型扩束系统。系统要求在1 550 nm、1 064 nm、800 nm和632.8 nm激光波段,全视场范围内波像差RMS不大于0.1（=632.8 nm）,且无中心遮拦。通过计算初始结构参数,利用Zemax软件优化,采用4片反射式非球面进行设计,全系统体积约为9010060 mm3,波像差最大为0.095,满足系统尺寸和像质要求,整个系统光能透过率约为92%,满足透过率大于85%的设计要求。     

Optical properties of a 5 m echelle vacuum spectrometer with an approximately diffraction-limited resolving power in the order of 106

The image formation and the spectral resolution of a 5m echelle spectrometer were investigated. As shown in this study, the spectrometer operates approximately diffraction-limited in the visible and uv, whereas in the vacuum uv (120.0 nm) the resolving power is still >54% of the diffraction-limited value. The spectrometer was designed according to the results of an analytical imaging theory. Residual optical aberrations were investigated by measuring the image distributions at four wavelengths between 120.0 and 632.8 nm (grating replaced by a plane mirror), in order to experimentally test the reliability of these theoretical results in combination with the influence of the imperfections of the optical components. The ratios of 40%-widths of the measured image distributions in the exit slit plane to the corresponding theoretical values were determined to be 0.56 at 120.0 nm, 0.68 at 174.0 nm, 0.74 at 257.3 nm, and 0.99 at 632.8 nm. Due to a lack of suitable light sources in the vacuum uv with sufficiently small band widths, the instrumental functions of the spectrometer could only be measured at 257.3, at 514.5, and at 632.8 nm, using stabilized and frequency doubled laser lines. The resolving powersR, which were deduced from the 40%-widths of the measured instrumental functions, were determined to be 1.42×10⁶ [0.80] at 257.3 nm, 0.86×10⁶ [0.97] at 514.5 nm, and 0.71×10⁶ [0.98] at 632.8nm (ratiosR ^exp/R ^theor in brackets). The comparatively high resolving powerR≳0.02×10⁶ [0.54] at 120.0 nm was estimated from the 40%-width of the measured image distribution.     

超高阈值Pick-off反射镜的研制

 采用水中抛光技术抛制了90mm×60mm×10 mm的K₉玻璃基片,表面粗糙度达1nm。在APS1504镀膜机上,摸索了电子束蒸发镀膜的最佳工艺条件,较稳定地在该超光滑玻璃表面上镀制了对波长1054 nm、入射角45°、反射率R≥99.5%的反射膜。膜层的抗激光损伤阈值可达26 J/cm²(1054nm, 1ns),镀膜后该玻璃基片反射波前可达l /10(p-v),最终制备了超高阈值Pick-off反射镜。     

Experimental Study on Optical Limiting and Transient All-optical Switching Properties of a Cubanelike Transition-metal Cluster Compound (n-Bu4N)3[MoAg3BrI3S4]

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Visible and near-infrared optical properties of Nd:CLNGG crystal waveguides formed by proton implantation

A Nd:CLNGG waveguide structure operated at wavelengths of both 632.8 nm and 1539 nm was demonstrated for the first time to our knowledge, which was produced by the 480-keV H~+ion implantation with a dose of 1.0×10~(17)protons/cm~2.Its propagating modes at 632.8 nm and 1539 nm were measured by the well-known prism coupling technique. The refractive index profile at either 632.8-nm wavelength or 1539-nm wavelength was optical barrier type in the proton-implanted Nd:CLNGG crystal optical waveguide, which was calculated by using the reflectivity calculation method. The near-field light intensity distributions were also simulated by the finite-difference beam propagation method in the visible and nearinfrared bands.     

IRRADIATION OF HUMAN LYMPHOCYTES WITH He-Ne LASER INCREASES THE BLAST Ⅰ TRANSFORMATION CAUSED BY PHYTOHEMAGGLUTSNIN

The irradiation of human lymphocytes with a He-Ne laser(632.8nm,56J/m~2) elevated the DNA synthesis levol in phytohemagglutinin-treated cells,but didnot itself cause the blasttransformation.The boosting effect of irradition was especiallypronounced in case of suboptimal PHA concentrations(0.5and 1μg/ml).     

Multiexcitation Raman Spectroscopy in Identification of Chinese Jade

The high-fluorescence background of jade creates a great impact on the Raman spectra measurements that impedes their application in jade analysis and treatment, particularly with ancient jade. The five most important materials of Chinese ancient jade are amphibole, serpentine, turquoise, agate/chalcedony, and anorthite-zoisite (Dushan jade). This study comparatively analyzed the Raman spectra of different wavelengths' excitation light sources (514.5 nm, 632.8 nm, 785 nm) in identifying these Chinese jades, and this article discusses the most applicable ones to the analysis of different jade materials. The results show that although 632.8 nm He-Ne laser is appropriate for turquoise jades, generally speaking, Raman spectra produced by the 785 nm semiconductor laser and the 632.8 nm He-Ne laser are better for most kinds of jades than the spectra produced by the 514.5 nm argon ion laser, and both of them can be effectively used jointly in research by nondestructive phase analysis of Chinese ancient jade.