低功率激光热透镜效应的模拟及研究

与高功率激光相比,低功率激光更安全,其热透镜效应对激光功率变化更敏感,更适合用于实验教学.本文利用有限元法模拟低功率激光的热透镜效应,模拟介质温度场和等效热透镜焦距,定量探究低功率激光热透镜焦距与激光功率以及介质热吸收率、厚度的关系.模拟结果与实验数据符合良好,为探究低功率激光热透镜效应实验提供理论依据.     

基于级联跃迁的2.8 μm低掺铒氟化物光纤激光器数值分析与优化

2.8 μm和1.6 μm激光级联跃迁的工作方式,可以有效解决低掺铒氟化物光纤中自终止效应导致的2.8 μm激光功率提升难题.建立基于低掺铒氟化物光纤2.8 μm和1.6 μm激光级联跃迁的中红外光纤激光器数值模型,系统分析了2.8 μm和1.6 μm激光波长对2.8 μm激光功率和转换效率的影响.计算结果表明,选取1610 nm作为级联激光工作波长,能有效平衡2.8 μm激光下能级⁴I_13/2粒子向基态⁴I_15/2和激发态⁴I_9/2的跃迁过程,实现2.8 μm波段激光输出功率和效率的提升.此外,计算了1.6 μm激光腔反馈对2.8 μm激光功率和效率的影响,结果表明,仅通过光纤端面提供的弱反馈即可实现1.6 μm激光振荡,从而获得高效率2.8 μm激光输出.     

不同功率下激光重熔对Mg-Zn-Y-Zr合金性能的影响研究

由于镁合金耐磨及硬度性能较差,应用激光重熔技术进行表面改性就显得尤为必要,其中激光功率因素所产生的影响十分显著。为了探究激光重熔中功率因素对稀土镁合金的微观组织结构,硬度以及摩擦磨损性能的影响。通过使用3kW的DILAS半导体激光器对Mg-1.85Y-7.91Zn-0.75Zr(质量分数,%)合金进行不同功率下的激光重熔实验。采用光学显微镜(OM),电子扫描显微镜(SEM),X射线衍射仪(XRD)和能谱仪(EDS)观察所制得试样的组织,形貌,相成分及分布;使用显微硬度计测量维氏硬度;使用摩擦磨损试验机测试样品的摩擦磨损性能,从而得出不同激光功率对组织,性能的影响。研究表明,经过重熔处理的合金宏观凝固组织明显细化,且随着功率升高,晶粒变大,第二相分布愈加弥散。由于细晶强化,固溶强化以及弥散强化的影响导致了硬度和耐磨性提高,其中800,1000,1200,2000W激光功率作用下重熔细晶区的维氏硬度平均值分别为90.97,93.47,94.20,95.53HV,而粗晶基材区的维氏硬度平均值仅为63.90HV,2000W功率作用下的硬度照比基材提升了49.50%。随着功率的升高,耐磨性越高且逐渐从以黏着磨损为主过渡到以磨粒磨损为主。可见,激光重熔技术可以明显强化该稀土镁合金,激光功率的增大可以显著增加该合金的硬度以及抗摩擦磨损性能。     

调Q CO_2激光功率放大器的输出特性

利用描述CO_2激光器动力学过程的六温度模型理论,建立了计算调Q CO_2激光功率放大器输出特性的数学模型,进行了理论分析和数值计算,并讨论了分光比等参数对输出脉冲特性、输出光谱的影响。结果表明:该调Q CO_2激光功率放大器存在临界增益长度和临界光强分束比,低于临界值时无法获得激光输出;该调Q CO_2激光功率放大器的输出激光脉冲波形、峰值功率、脉冲宽度、输出光谱与光强分束比、抽运电子数密度等参数有关,光强分束比越小,输出的调Q激光脉冲宽度越大,峰值功率越低;该调Q CO_2激光功率放大器利用Q调制的高增益特性,通过控制调Q元件所在的低功率支路可以实现高平均功率的调Q脉冲CO_2激光输出,很好地解决了调Q CO_2激光功率放大器难以高功率运转的问题。     

多孔硅的拉曼光谱研究

本文研究了多孔硅的拉曼光谱随激发激光功率的变化 ,发现当激发光的功率较低时 ,多孔硅的拉曼光谱在 5 2 0cm- 1附近为一单峰。随着激光功率的增加 ,该单峰向低波数移动且半高宽增大 ,当继续增大激光功率时 ,该单峰分裂为双峰 ,位于低波数一侧的拉曼峰随着激光功率的增大而进一步向低波数移动。多孔硅的拉曼光谱随着激光功率的变化是一个可逆的过程。这一结果表明 ,低波数拉曼峰的位置既不能作为多孔硅颗粒尺寸的量度 ,也不能只把低波数的拉曼峰作为多孔硅的特征。我们认为激光诱导多孔硅中LO和TO声子模的简并解除是观察到双峰的主要原因。     

低强度He-Ne激光照射巨噬细胞对其免疫活性的影响

利用新型化学发光试剂MCLA,通过光学方法,并改变激光功率和照射时间研究了低强度HeNe激光照射巨噬细胞对其免疫活性影响实验结果表明,巨噬细胞在适当的激光功率和照射剂量下可大大提高其免疫活性,而过大或过小的激光功率或照射剂量则不能激活其免疫活性的显著提高,甚至产生明显的抑制效应.     

利用金刚石探测器测量软X光辐射功率

使用天然Ⅱａ型金刚石光电导探测器（ＰＣＤ），测量激光等离子体发射的软Ｘ光辐射。由于探测器在２００ｅＶ～２２００ｅＶ之间具有平响应特性，可以不加滤片直接测量Ｘ光功率和能量。金刚石ＰＣＤ与软Ｘ光能谱仪和平响应Ｘ光二级管的测量结果基本一致。     

激光烧蚀硅基表面抗反射微结构的声信号监测

为了提高抗反射硅表面制备的加工质量、缩短研制周期,提出了一种基于时频域处理的面向激光加工过程的声波信号在线监测及分析方法。利用声信号的时频谱图分析了0～30 kHz内的声信号与激光烧蚀形成的表面微结构特征尺寸之间的相关性,具体分析了激光功率及加工次数对微结构深度及声信号各频率幅值变化的影响。以声信号作为输入,基于人工神经网络对加工质量进行预测。实验结果表明：通过监测激光加工时产生的声信号能够明确反映被烧蚀硅表面是否形成周期性微结构,且微结构宽度不同,其对应的声信号频率组成也不同。在微结构宽度固定的情况下,归一化后的声信号特征参数随微结构深度线性变化,且受到激光功率变化的影响忽略不计。以硅基表面5%的反射率作为加工质量分界线,采用人工神经网络对加工质量的预测结果与实际测量结果的准确率可以超过90%。结果表明：声波在线监测可以有效应用于评估表面加工质量,为抗反射硅表面制备过程的实时监测提供了理论依据。     

FP腔中光驱动微悬臂的双稳效应的研究

研究了高灵敏度悬臂梁与光纤端面构筑的低精细度FP型光腔中光驱动的悬臂梁振动的双稳效应。通过改变输入到光腔内的激光功率,检测与之相应的悬臂梁的形变。在实验中发现悬臂梁的形变随激光功率的改变呈现非线性变化的关系,在激光功率增大到一定闽值时可以诱导产生光力双稳效应。通过改变光腔初始腔长成功实现了对产生光力双稳效应阈值的调节。     

激光诱导多孔硅晶格畸变的Raman光谱和光致发光谱研究

研究了掺钛水热法制备多孔硅的Raman光谱和光致发光谱.实验发现,当激光功率较低时,多孔硅的Raman光谱在略低于520cm^-1附近表现为一锐的单峰,和晶体硅的Raman光谱类似.随激光功率增大,该单峰向低波数移动,Raman和光致发光峰的强度与激光强度的一次方成正比.当激光功率增大到一定值时,该单峰分裂成两个Raman峰,光致发光谱的强度突然增大,与激光强度之间不再满足一次方的关系,位于低波数一侧的Raman峰随激光功率增大进一步向低波数移动.多孔硅Raman光谱随激光功率的变化是 关键词： 多孔硅 Raman光谱 光致发光     

Pulse-Width Jitter Measurement for Laser Diode Pulses

Theoretical analysis and experimental measurement of pulse-width fitter of diode laser pulses are presented. The expression of pulse power spectra with all amplitude jitter, timing jitter and pulse-width jitter is deduced. The power spectra with and without pulse-width fitter are that the pulse-width jitter will contribute considerably numerically simulated. The simulation results indicate noise to the pulse power spectrum while the product of pulse width and angular frequency is larger than 1. The experimental measurement of pulse-width fitter of a gain-switched Fabry-Perot laser diode with 2.4 GHz repetition rate is also reported. In comparison of the noise power spectra of the first, fourth and seventh harmonics of the pulse repetition rate, 2.3ps pulse-width jitter is obtained.     

Photoacoustic detection of two photon absorption in formaldehyde using pulsed dye laser

Absorption spectra of formaldehyde molecule in the gas phase have been recorded using photoacoustic (PA) technique with pulsed dye laser at various power levels. The spectral profiles at higher power levels are found to be different from that obtained at lower laser powers. Two photon absorption (TPA) is found to be responsible for the photoacoustic signal at higher laser power while the absorption at lower laser power level is attributed to one photon absorption (OPA) process. Probable assignments for the different transitions are given in this paper.     

Influence of terahertz laser radiation on the spectral characteristics and functional properties of albumin

The exposure of albumin (transport protein of blood serum) to laser radiation with a frequency of 3.6 THz resulted in a change in the intensity of characteristic bands in UV absorption spectra and in circular dichroism spectra. These changes depend on the exposure duration and the laser radiation power and indicate conformational changes in protein molecules.     

High power single transverse mode operation of a tapered large-mode-area fiber laser

To get high output power with good beam quality, a tapered section is introduced to large-mode-area (LMA) Yb-doped fiber laser. Output characteristics of the fiber laser without tapered section and with tapered section are compared experimentally. When the launched pump power is 119.1 W, 77.9 W with M² 3.08 and 56.4 W with M² 1.14 can be obtained, respectively. The corresponding slope efficiencies are 71.8% and 54.1%, respectively. Although output power of the tapered fiber laser has 30.6% penalty, brightness of it is as much as 5.28 times of the fiber laser without tapered section. Moreover, spectra of them are measured. It is found that tapered section makes lasing wavelength of the fiber laser shorter.     

入射激光功率对硅纳米线拉曼光谱及荧光光谱的影响

一维纳米材料硅纳米线是目前重要的光电材料之一,采用化学气相沉积法制备了硅纳米线,实验研究了不同功率532 nm激光激发下的拉曼光谱和荧光光谱,随着入射激光功率的增加,一阶拉曼光谱出现红移和非对称加宽,而且红移同入射激光功率成正比,光致荧光光谱出现蓝移和双峰结构。使用声子限域效应、应变效应和激光非均匀加热效应对实验结果进行了分析,并采用matlab模拟了入射激光功率同拉曼频移的理论关系曲线,结果表明激光非均匀加热效应是引起拉曼光谱和光致荧光光谱变化的主要原因。     

Diode-end-pumped Tm:GdVO4 laser operating at 1818 and?1915?nm

High power operation at 1818 and 1915 nm has been demonstrated from a Tm:GdVO₄ laser operating in quasi-continuous-wave mode with a maximum measured power of 8.7 W and a laser output energy of 175 mJ was observed in a 20 ms pulse at 1.9 μm. The operation at 1818 nm is the shortest wavelength achieved at multi-watt power levels for a Tm-doped solid-state laser without intra-cavity tuning elements. It has been shown that by careful analysis of the emission spectra, the Tm:GdVO₄ laser can be tuned over a 100 nm wavelength range simply by appropriate selection of the reflectivity of the output coupler.     

Effect of pump power on the tuning range of a filterless erbium-doped fiber ring laser

In this paper, we establish the influence of pump power on the tuning characteristics of a filterless erbium-doped fiber laser, operating in the L band. Tunable action is achieved with the control of intra cavity loss. The explicit dependence of tunability on the average inversion levels is brought out. The shift in the lower limit of tuning range and the non-linear dependence of lasing wavelength on the intra cavity loss are analytically deduced using the gain spectra and experimentally interpreted using amplified spontaneous emission spectra. Continuous tunability is achieved with the careful control of pump power. PACS 42.55.Wb; 42.60.Da; 42.55.-f     

Effects of the agglomeration state on the Raman properties of Co3O4 nanoparticles

The features of the Raman spectra of Co₃O₄ 30‐nm nanoparticles depend strongly on their agglomeration state. When measured at low incident laser power, the spectrum of isolated nanoparticles corresponds to that found in bulk materials, whereas the agglomerated nanoparticles present a clear red‐shift and broadening of the Raman bands. On the other hand, when measured at even lower power, both agglomerated and isolated nanoparticles show the same spectrum of microscopic particles. These effects have been studied by variations of the 532‐nm laser power and the environmental temperature. The thermal dependence of Raman spectra of agglomerated nanoparticles is different to that of isolated nanoparticles but is comparable to the one of bulk material. The different behaviour of the nanoparticles at different agglomeration state is associated to the transmission of phonons among the particles. On the other hand, an increase of the laser power causes a larger number of acoustic phonons, producing a variation of the vibration anharmonicity of the nanoparticles. This increase is more pronounced in the agglomerated nanoparticles, due to the transmission of phonons, causing a much intense modification of the Raman spectrum produced by the laser power. These results clearly indicate that the agglomeration state of the nanoparticles affects their Raman properties. Copyright © 2012 John Wiley & Sons, Ltd.     

激光大气闪烁的小波频谱分析

激光对数光强起伏的快速傅里叶变换功率谱的无标度区间的标度指数在许多情况下很不稳定,并且超出了理论界限,因而本文引入了离散小波变换（ＤＷＴ）频谱分析。通过对１／ｆ信号的快速傅里叶变换频谱和离散小波换频谱的对比分析,验证了离散小波变换频谱分析的优越性。激光大气闪烁的离散小波变换频谱的无标度区间的标度指数在一天内（除日出后和日落前两段时间外）的变化比较稳定,并且超出理论界限。这此结果表明,对于一般在大气     

Comparison of surface films formed on titanium by pulsed Nd:YAG laser irradiation at different powers and wavelengths in nitrogen atmosphere

The nitridation of titanium (Ti) caused by a Q-switched Nd:YAG laser under nitrogen gas atmosphere was investigated in situ using X-ray photoelectron spectroscopy (XPS). A laser having a wavelength of 1064 nm and 532 nm (SHG mode) was irradiated on a titanium substrate in an atmosphere-controlled chamber, and the substrate was then transported to an XPS analysis chamber without exposing it to air. The characteristics of the surface layer strongly depend on the laser power. When the power is relatively low, a titanium dioxide layer containing a small amount of nitrogen is formed on the substrate. Laser irradiation beyond a certain laser power is required to obtain a stoichiometric titanium nitride (TiN) layer. A TiN layer and an oxynitride layer with a TiO_xN_y-like structure are formed as the topmost and the lower surface layer, respectively, when the laser power exceeds this threshold value. The threshold laser power strongly depends on the wavelength of the laser, and this threshold value for the 532-nm laser is quite lower than that for the 1064-nm laser.