硅酸铅玻璃光敏性研究

采用四倍频的Nd∶YAG脉冲激光 (波长 2 6 6nm ,脉宽 10ns)对氧化铅摩尔分数在 0 3至 0 5的硅酸铅玻璃体样品进行照射 ,并对照射前后样品的折射率及紫外可见吸收光谱进行了测量。研究发现不同能量密度的2 6 6nm激光照射硅酸铅玻璃体样品 ,会使样品的紫外可见吸收光谱产生不同的变化 :当 2 6 6nm激光能量密度较高时 (15 0mJ/cm2 ) ,样品在可见区域的吸收系数明显增大 ,样品表面会产生褐色斑点 ;而当 2 6 6nm激光能量密度较低时 (5 0mJ/cm2 ) ,尽管累计剂量较大 ,样品表面无斑点产生 ,吸收系数稍有增加 ,而折射率下降明显 ,最大Δn =- 0 .2 5± 0 .0 4。对氧化铅摩尔分数为 0 4 3的硅酸铅玻璃用不同能量密度的 2 6 6nm激光进行照射 ,发现当激光能量密度大于某一阈值时 ,样品在可见区域的吸收系数突然增大 ,这可能是由于硅酸铅玻璃吸收 2 6 6nm激光能量导致局部温度升高而引起玻璃结构改变所致。     

应用激光质谱法选择探测一氧化碳

此文解决了激光质谱法中从含同质量数的N2分子的混合气体中选择CO分子这一问题,由于用紫外266nm激光不能从含N2分子的混合气体中选择CO分子,因此采用了可见激光来探测,发现用可见激光430～435nm的激光能成功地将CO分子选择探测出来。此外还着重分析了在可见波段和266nm激光下产生CO+离子的机理：在可见光波段443.55nm所对应的共振峰是CO分子吸收3光子的激光能量与A1Π态的振动量子数为2的振动态共振产生的;434.3nm所对应的共振峰是CO分子吸收3光子的激光能量与A1Π态的振动量子数为3的振动态共振产生的;CO分子吸收两光子的266nm激光能量与A1Π态第7振动态的某一高转动态相共振,处于该振动态的CO分子再继续吸收一个光子的266nm激光的能量至其电离态电离产生CO+离子。     

六硝基菧的紫外光解

采用紫外-可见光谱、X-射线光电子能谱、电子自旋共振谱及质谱等实验手段研究了固态含能材料六硝基菧（HNS）在365 nm紫外光照下的光解机理。HNS的乙腈溶液被紫外光照射后,在310 nm和350 nm处出现了两个新的吸收峰。X-射线光电子能谱实验中,N元素和O元素的窄谱图分别在401 eV和528 eV处出现了新峰。质谱分析则显示在质荷比403和329处出现了两个新的特征离子峰。实验结果表明:CNO2键断裂、分子中NO2基团异构化为亚硝基,以及随后的NO消去等过程均可能发生在六硝基菧的紫外光解反应过程中。     

射频磁控共溅射GaAs/SiO2纳米颗粒镶嵌薄膜的光学性质

应用射频磁控共溅射方法和真空退火方法制备了GaAsSiO2纳米颗粒镶嵌薄膜.X射线衍射实验结果表明,经高温退火的薄膜中形成了面心立方闪锌矿结构的GaAs纳米晶粒,晶粒平均直径为1.5—3.2nm.吸收光谱展示了由于强量子限域引起的1.5—2eV的吸收边蓝移.室温光致荧光(PL)光谱显示了电子重空穴激子与电子劈裂空穴激子的近紫外和紫外双PL谱峰以及深俘获态的PL谱峰.对实验吸收边蓝移量与有效质量模型的蓝移量的悬殊差别、俘获态PL谱的形成以及PL谱线的特征作了解释.应用激光Z扫描技术测量了退火温度为500℃的复合膜在非共振条件下的光学非线性,结果表明,复合膜的非线性折射率系数和非线性吸收系数都比块材GaAs相应的系数增大了5个数量级.光学非线性系数增大主要起因于强量子限域效应 关键词： 射频磁控共溅射 GaAsSiO2纳米颗粒镶嵌薄膜 光谱 激光Z扫描     

金属纳米团簇复合薄膜Au/BaTiO3与Fe/BaTiO3的PLD制备及其光吸收特征

用脉冲激光沉积技术制备了掺杂纳米金属颗粒Au或Fe的BaTiO₃复合薄膜.用透射电子显微镜和x射线光电子能谱表征了金属颗粒的形态和化学态.330—800nm范围的吸收谱研究表明，掺Au颗粒的BaTiO₃薄膜在580nm附近有一个明显的共振吸收峰，而掺Fe颗粒的BaTiO₃薄膜没有这样的吸收峰.用Mie散射理论对结果进行了分析. 关键词： 复合薄膜 金属颗粒 脉冲激光沉积 吸收谱     

金属纳米团簇复合薄膜Au/BaTiO3与Fe/BaTiO3的PLD制备及其光吸收特征

用脉冲激光沉积技术制备了掺杂纳米金属颗粒Au或Fe的BaTiO3复合薄膜.用透射电子显微镜和x射线光电子能谱表征了金属颗粒的形态和化学态.330-800nm范围的吸收谱研究表明,掺Au颗粒的BaTiO3薄膜在580nm附近有一个明显的共振吸收峰,而掺Fe颗粒的BaTiO3薄膜没有这样的吸收峰.用Mie散射理论对结果进行了分析.     

特殊变色蓝宝石的紫外-可见光光谱研究

坦桑尼亚Umba出产颜色丰富的刚玉,该研究对象是一颗来自Umba的具有特殊变色效应的蓝宝石,D65光源（色温6 500 K）下呈现淡黄色,A光源（色温2 856 K）下呈现淡紫红色。为了研究这颗变色蓝宝石紫外-可见光光谱中的谱峰归属与变色成因,该研究使用电荷补偿理论来分析此样品紫外-可见光光谱中的谱峰归属。采用紫外-可见分光光度计（UV-Vis）和激光剥蚀电感耦合等离子体质谱仪（LA-ICP-MS）对这颗变色蓝宝石进行了测试。结果发现,变色蓝宝石紫外-可见光光谱中存在位于377,388和450 nm处的3个吸收峰和1个以560 nm为中心的宽缓吸收带。样品的颜色主要受450 nm处吸收峰和以560 nm为中心的吸收带影响,其中以560 nm为中心的吸收带造成了这颗蓝宝石的变色效应。根据激光剥蚀电感耦合等离子体质谱仪的测试结果,样品中主要杂质元素有Fe,Ti,Cr,V和Mg等。样品紫外-可见光光谱中377,388和450 nm处的吸收峰是由Fe3+导致。蓝宝石中的Cr3+,V3+,Fe2+-Ti4+对都可以在560 nm附近产生吸收,结合电荷补偿理论分析,刚玉中的Mg2+会优先和Ti4+进行电荷补偿,样品中Mg含量要稍微高于Ti,推测样品中几乎所有Ti4+会与Mg2+进行电荷补偿,因此样品中几乎不会存在Fe2+-Ti4+对。Fe2+-Ti4+对电荷转移产生的吸收特征具有很强的偏振性,尤其是在580 nm以后的吸收特征会随着偏振方向的改变而有很明显的变化。偏振紫外-可见光光谱测试发现以560 nm为中心的吸收带没有明显的偏振性,进一步验证了样品中几乎没有Fe2+-Ti4+对,因此以560 nm为中心的吸收带主要是由于Cr3+和V3+造成的。样品的颜色主要是由Fe3+,Cr3+和V3+引起的,而变色效应主要是由Cr3+和V3+导致。结合电荷补偿机制与偏振-紫外可见光光谱来解释这颗变色蓝宝石的紫外-可见光光谱中以560 nm为中心的吸收带的归属,为研究刚玉紫外-可见光光谱中较为常见的位于560 nm左右吸收带的归属提供了一种新的研究思路。     

准波导结构下染料薄膜的荧光光谱和放大自发辐射光谱特性

通过对RhB/PMMA和Rh6G/PMMA染料薄膜的荧光光谱和放大自发辐射(ASE)光谱的实验测量和理论分析,研究了准波导结构染料薄膜的荧光光谱和ASE光谱特性。实验上采用连续激光和脉冲激光照射,分别测量准波导结构RhB/PMMA和Rh6G/PMMA染料薄膜的荧光光谱和ASE光谱,发现荧光峰和ASE峰随着染料掺杂浓度和薄膜厚度的增加产生红移;理论上考虑准波导结构下薄膜中染料的自吸收效应,类比激光器谐振腔模型,分析低阶导模传输的增益特性,获得了荧光光谱与ASE光谱中荧光峰和ASE峰对应波长与染料掺杂浓度的关系,数值计算与实验测量相吻合。结果表明,准波导结构下薄膜中染料自吸收效应导致荧光峰及ASE峰发生红移,改变染料掺杂浓度,可以在较大调谐范围实现ASE。     

非晶态As_2S_8半导体薄膜的光激励现象的研究及应用

实验研究了非晶态As2S8半导体薄膜在紫外汞灯和He_Cd激光照射下的光诱导现象,证实了光照射后的As2S8薄膜的折射率增大,体积缩小,可见光吸收谱的吸收带蓝移。在此基础上,应用光折变效应试制了As2S8条波导,观测到As2S8条波导的光阻断效应,实现了光_光效应的开关功能。     

不同浓度掺铊碘化铯(CsI:Tl)晶体的光谱特性

对含有不同浓度Tl+激活剂的CsI:Tl晶体进行了光吸收光谱和荧光光谱测量,以研究CsI:Tl的光学吸收和发光特性.实验观察到,在紫外吸收谱中包含有三个特征结构峰297,273和247 nm,高浓度Tl+晶体的吸收结构峰比低浓度的峰明显加宽,其中A吸收峰297 nm红移20 nm.室温下不同能量紫外光激发的荧光带形状相同,不受Tl+浓度影响.分析认为,晶体中掺杂Tl+后品格畸变是导致吸收峰或荧光激发峰变化的主要原因,但对发光带峰宽和峰位影响不明显.     

Femtosecond Laser Induced Rewritable Optical Memory in Silicate Glasses

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Femtosecond Laser Induced Rewritable Optical Memory in Silicate Glasses

A novel method for producing rewritable optical memory with ultra-high storage density and ultra-high recording and readout speed is presented. A 120 fs, 800 nm, 1 kHz laser focused by an objective lens is used to produce recording bits in glass with high transmittance contrast. These recording bits can be erased by heat-treatment. The mechanism has been discussed by means of the absorption and electron spin resonance(ESR) spectra of silicate glasses before and after irradiation by the laser. The absorption of glasses increases greatly after irradiation because of color-center generation through multi-photon absorption. ESR spectra shows that the color-center induced in the glass are hole-trapped defects. The color-center disappears when the glass heated because the holes and electrons at traps are released by thermal stimulation and recombine again.     

Composition dependence of the photoinduced refractive-index change in lead silicate glasses

A large photoinduced refractive-index change (as great as Dn=0.21+/-0.04) is obtained in lead silicate glasses by irradiation with the frequency-quadrupled output of a Q -switched YAG laser (266 nm). An approximately exponential relationship is found between the photoinduced refractive-index change and the lead cation mole fraction over the composition range from 18.7% to 57%. The induced refractive-index change is permanent and shows no decay after heating to 360 degrees C during 1 h. Dispersion of the refractive-index change suggests that the photosensitivity is associated with changes in the intrinsic glass absorption edge.     

Laser-induced birefringence in optical glasses

Laser-induced birefringence in silicate glasses is investigated. The birefringence is found at the boundary between the irradiated and unirradiated regions in the glass after long-term exposure to N₂ laser radiation (λ = 337 nm). Along with the stationary effect, a temporal (transient) change in the polarization of the probe beam is also observed, which arises only during UV irradiation and vanishes when the irradiation is over. The birefringence found is explained by the occurrence of anisotropy at the boundary between the irradiated and unirradiated regions of a glass due to a local change in the glass density in the irradiated region.     

Ge：SiO2的光敏缺陷的研究

研究了Ｇｅ；ＳｉＯ２光敏缺陷的特性，分别在４８８ｎｍＡｒ离子激光与１９３ｎｍＡｒ准分子激光作用下，由紫外吸收带，激光荧光的测量实验及电子自旋共振实验，发现光纤中５．１ｅＶ锗缺陷吸收带实验上是由５．０６ｅＶ可光致漂白带与５．１７ｅＶ不可漂白带组成；２９５ｎｍ的激发荧光与５．０６ｅＶ的缺氧锗缺陷对应，随５．０６ｅＶ缺陷吸收带的漂白而衰减；     

Luminescence properties of silver zinc phosphate glasses following different irradiations

We report on exposing a photosensitive zinc phosphate glass containing silver to different radiation (electron, gamma, optical). Laser irradiations using nanosecond ultraviolet (UV) and femtosecond infrared (IR) laser are compared with gamma and electron exposure. All irradiated glasses exhibit absorption maxima around 320 nm and 380 nm and emission in the visible spectral range. Following exposure, silver clusters are formed. The optical response of such species is investigated using absorption and fluorescence spectroscopic techniques. The mechanism of formation of these clusters is discussed.     

Z-scan study of nonlinear absorption of gold nano-particles prepared by ion implantation in various types of silicate glasses

Metal nano-clusters composite glasses synthesized by ion implantation have been shown as promising nonlinear photonic material. In this paper, we report on the nonlinear absorption measurements of gold nano-particles implanted in four structurally different types of silicate glasses. All targets containing gold nano-particles in a layer 500 nm under the surface of the glass have been prepared by ion implantation with subsequent annealing. The targets were characterized by UV–VIS absorption spectroscopy, transmission electron microscopy (TEM) and by the Z-scan technique. The resulting nano-particles differed in size, range of particle size and shape as well as depth distribution characteristic for glasses with different chemical compositions. With the Z-scan technique, it can be shown that the nano-particles produced in silicate glasses exhibit substantial two-photon absorption (TPA). The TPA coefficient differed depending on size, shape, and depth distribution of the metal nano-clusters and the structure and composition of the glass substrates. The highest TPA coefficient (16.25 cm/GW) was found for the glass BK7 in which the largest non-spherical nano-particles have been observed in the thinnest layer.     

Doping transition metal ions as a method for enhancement of ablation rate in femtosecond laser irradiation of silicate glass

We present a doping method to improve the femtosecond laser ablation rate and promote ablation selectivity. Doping transition metal ions, Co2＋ or Cu2＋, in silicate glass apparently change absorption spectroscopy and induce resonant absorption at wavelengths of 600 and 800 nm, respectively. Comparing with femtosecond laser processing of the same glass without doping, we find that the threshold fiuenee decreases and the ablation rate increases in resonant absorption in doped silicate glass. Resonant absorption effectively increases multiphoton ionization for seed-free electron generation, which in turn enhances avalanche ionization.     

Nonlinear photoionization and laser-induced damage in silicate glasses by infrared ultrashort laser pulses

We show that photoionization of wide band gap silicate glasses by infrared ultrashort laser pulses can occur without laser-induced damage. Two glasses are studied, fused silica and a multi-component silicate photo-thermo-refractive (PTR) glass. Experiments are performed by low numerical aperture focusing of ultrashort laser pulses (100 fsec<τ<1.5 psec) at the wavelengths 780 nm, 1430 nm, and 1550 nm. Filaments form inside both glasses and are visibly observable due to intrinsic luminescence. Keldysh’s theory of nonlinear photoionization is used to model the formation of filaments and values of about 10¹³ W cm⁻² for the laser intensity and 10¹⁹ cm⁻³ for the free electron density are estimated for stable filaments to arise. Laser-induced damage is studied by the generation of a third harmonic from an interface created between a damage site and the surrounding glass matrix. It is found that third harmonic generation occurs only after several thousands of laser shots indicating that damage is not a single-shot phenomena. The ability to photoionize PTR glass without damage by ultrashort laser pulses offers a new approach for fabricating diffractive optical elements in photosensitive glass.