355 nm激光烧蚀LiMn2O4反应产物的飞行时间质谱

采用角分辨飞行时间质谱法研究了355 nm脉冲激光烧蚀LiMn2O4的反应. 在较低激光能量密度(0.8 J·cm^-2)测得的离子和中性烧蚀产物主要有Li, O, LiO, LiO₂ , Mn, Li₂, Li₄, Li₆, LiMn, MnO, MnO₂等. 激光能量密度较大时, 烧蚀产物中的氧化物不仅相对量增加, 而且物种更加丰富. 它们的飞行时间谱可用带质心速度的Maxwell-Boltzmann分布函数拟合. 烧蚀产物Li, LiO, LiO₂ 和 Mn存在能量密度表观阈值, 并且离子产物的阈值比相应的中性产物高. 烧蚀产物中原生离子和中性产物的空间角分布可用cosⁿ θ 或θ cosθ+(1-δ)cosⁿθ拟合. 此外, 对355 nm脉冲激光对LiMn₂O₄的烧蚀机理进行了讨论.     

同位索峰型计算在归属多元素团簇质谱中的应用

介绍了一种通过计算分子的同位素丰度模拟质谱峰型，根据比较质谱峰的位置和形状来帮助归属多元素团簇的飞行时间质谱的方法。这种方法不仅有助于归属完全分辨的低质量离子峰，还能从重叠的质谱峰中确定各个组份的相对含量。最后介绍了如何用这种方法来分析激光烧蚀ＭｎＣｌ２·４Ｈ２Ｏ和ＣｕＣｌ２·２Ｈ２Ｏ得到的正负团簇离子质谱     

低温基体隔离Mn2（CO）10的紫外激光光解

采用２８０ｎｍ和３５５ｎｍ的脉冲激光作光解光源，由ＦＴＩＲ进行初级产物探测，研究了Ｍｎ２（ＣＯ）１０在低温基体隔离条件下的光解反应。结果表明，在Ａｒ基体中，Ｍｎ２（ＣＯ）１０经２８０ｎｍ激光光解的初级产物主要是Ｍｎ２（ＣＯ）９；而在Ｘｅ基体中还观察到了Ｍｎ（ＣＯ）５的生成；与２８０ｎｍ激光相比，采用３５５ｎｍ激光光解Ｍｎ２（ＣＯ）１０，Ｍｎ２（ＣＯ）９的产率较低。     

用飞行时间二次离子质谱法分析模塑料成分

用飞行时间二次离子质谱（ＴＯＦ－ＳＩＭＳ）结合银离化的方法研究了集成电路封装中常用的环氧模塑料的两种主要成分：邻甲酚环氧树脂和线型酚醛树脂。测得ｎ＝０～４的环氧树脂分子及相应的水解成分和ｎ＝１～７的酚醛树脂分子。碎片离子中除了芳香化合物的特征碎片外,还有反映树脂结构的碎片。通过对环氧树脂银离化碎片离子的分析,推断中间苯环上的侧链是最可能断裂的     

O2气中激光烧蚀Ta2O5产物离子的氧化反应

Ta2O5薄膜作为电容元件材料的替代品已在微电子等领域中显示出广阔的应用前景[1]．脉冲激光沉积（PLD）法制备Ta2O5薄膜以其显著的优点引起了广泛重视[2，3]．而对激光烧蚀的物理化学过程的认识是完善这一方法的重要前提．我们曾采用时间分辨与角分辨飞行四极质谱[4]和发光光谱技术[5]较系统地研究了激光烧蚀Ta2O5产生的羽状物的组成和特征，并认为在O2气氛中沉积Ta2O5薄膜可以改善甚至避免形成缺氧的薄膜．但由于上述实验方法上的限制，未能详细考察激光烧蚀Ta2O5生成的离子产物在O2气氛中发生的氧化反应．为了研究激光烧蚀产物离子…     

α—氨基酸的快原子轰击质谱

本文研究了１８种α－氨基酸的快原子轰击质谱，发现添加三氟乙酸溶液能显著提高灵敏度，改善谱图。特征碎片主要有中性丢失ＣＯ２Ｈ２，Ｈ２Ｏ，ＮＨ３的离子以及Ｒ＾＋离子。侧链的性质决定了碎片的产生和离子的强弱。     

冷等离子体作用下CH4-CO2转化制合成气

在常常温压条件下,利用电晕放电,使ＣＨ４－ＣＯ２混合气转化生成合成气,结果表明,该过程中ＣＨ４和ＣＯ２的转化率与反应体系温量密度、原料气配比和流速等有关,在０．１ＭＰａ气压,能量密度为１０５０ｋＪ／ｍｏｌ（反应体系温度低于５００Ｋ）,ｎ（ＣＨ４）：ｎ（ＣＯ２）＝１：２条件下ＣＨ４和ＣＯ２的转化率分别超过６０％和５０％,超出了热力学平衡转化率的限制,通过调配原料的配比,可以得到不同ｎ（Ｈ２）／ｎ（ＣＯ）比值的产物,对该体系的反应机理进行了探讨。     

气相[（SiO2）nX]^—团簇产生机理

利用ＸｅＣｌ准分子激光烧蚀多种硅氧多孔结构材料，在负离子通道测得丰富的「（ＳｉＯ２）ｎＸ」＾－负离子团簇，并讨论了多孔网结构和表面活性基团的分布对激光能量的吸收，传输及团簇产生的重要作用。     

提高Nb2O5中Ta2O5光谱分析的灵敏度

由于Ｎｂ２Ｏ５与Ｔａ２Ｏ５物理、化学性质相似，主体Ｎｂ２Ｏ５对Ｔａ分析线强度干扰很大。因此，Ｎｂ２Ｏ５中光谱测定Ｔａ２Ｏ５的灵敏度很差，为了提高Ｔａ分析线强度，通常的光谱条件选择是无效的。实验表明在旋流气室中，采用高含量Ａｒ的（Ａｒ、Ｏ２）控制气氛电弧激发，提高了Ｎｂ２Ｏ５中Ｔａ２Ｏ５的光谱分析灵敏度。然而，由于Ｎｂ２Ｏ５在高温下易于被碳还原，虽然用Ｓｔａｌｌｗｏｏｄ喷咀可以改善蒸发，减慢样品还原     

含氮聚硅氧烷配位体及其与金属离子的络合作用

研究ｎ－β（氨乙基）－γ（氨丙基）三乙氧基硅烷［ＮＨ２（ＣＨ２）２ＮＨ（ＣＨ２）３Ｓｉ（ＯＥｔ）３］与二甲基二乙氧基硅烷［（ＣＨ３）２Ｓｉ（ＯＥｔ）２］共水解，制备含－（ＣＨ２）３ＮＨ（ＣＨ２）２ＮＨ２功能基的聚硅氧烷配位体。用ＩＲ、１ＨＮＭＲ和元素分析法对共聚产物的结构进行了分析，同时用紫外－可见光谱法和ＳＥＭ考察了共聚产物与Ｃｕ２＋等金属离子的络合作用。结果发现，两种单体进行了共水解反应，而且随着ＮＨ２（ＣＨ２）２ＮＨ（ＣＨ２）３Ｓｉ（ＯＥｔ）３比例增加，水解程度提高。共聚产物可以与Ｃｕ２＋离子形成稳定的络合物，但不能与Ｚｎ２＋离子或Ａｌ３＋离子形成稳定的络合物或螯合物。     

A time-resolved quadrupole mass spectrometric study on 355 nm laser ablated species ejected from LiMn2O4

Mass, velocity and angle distributions of the ablated species generated from 355 nm pulsed laser ablation of a LiMn2O4 target were investigated with an angle- and time-resolved mass spectrometric technique. Both neutral and ionic species of Li, O, LiO, LiO2, Mn, Li2, Li4, Li6, LiMn, MnO and MnO2 were observed at the laser fluence of 0.8 J · cm-2. The yield and variety of the ablated species increase with increasing the laser fluence. The time-of-flight spectra of ablated species can be fitted by a Maxwell-Boltzmann distribution with a center-of-mass velocity. There exist laser fluence thresholds for the ablated LiMn, Li2O and LiO2 species, and the fluence threshold of ionic species is higher than that of neutral species. The angular distributions of the ionic and neutral ablated species can be simulated by a cosnθor a bicosine function αcosθ+(1- α)cos"θ. In addition, the ablation mechanism of LiMn2O4 by a 355 nm pulsed laser is discussed.     

四极质谱法研究激光烧蚀Y1Ba2Cu3O7-δ产物的分布

采用空间和时间分辨的四极质谱法了３５５ｎｍ脉冲激光     

氯分子束与钛表面激光化学反应动力学

本文采用飞行时间质谱技术测定了在紫外(355nm), 可见(560nm)和近代红外(1064nm)脉冲激光作用下, 氯分子束与Ti表面反应产物的质量分布和速度分布。所得结果表明, 不同波长激光诱导反应的主要产物相同, 有Ti, TiCl, TiCl3和TiCl4。在高能量密度的紫外激光作用下, 首次测得具有很高动能的原生Ti+。各种含Ti氯化物的飞行时间谱, 能满意地用单组分或多组分Maxwell-Boltzmann公式拟合和分析。上述激光诱导气-固表面反应的机理主要由氯分子在Ti表面上的解离吸附,吸附态氯原子在表面上生成TiClx(X=1～4)的连串反应以及激光诱导脱附所组成。近红外激光主要引起热脱附, 而紫外激光的作用还原可能有非热脱附过程。     

超声分子束研究激光诱导Cl2和Ta表面反应动态学

本文研究了在三种不同波长的脉冲激光(365 nm, 560 nm和1064 nm)辐照下超声Cl_2分子束与多晶Ta表面的化学反应动态学. 由四极质谱和飞行时间增(TOF)测定了产物的质量分布和速度分布. 该反应的主要产物为TaCl, TaCl_2, TaCl_3及TaCl_4; 它们的TOF谱都可用Maxwell-Boltzmann分布拟合, 所得的平动温度分别在500 K—1500 K范围内. 测定了各种产物相对产率与激光能量密度和入的Cl_2分子平动能的关系. 此外, 对此气-固表面反应的机理进行了讨论。     

氯分子束与InP(100)表面反应散射的角分布研究

采用角分辨分子束散射技术研究了Cl_2与InP(100)表面热反应和激光诱导反应产物的角分布. 对于热反应, 由调制分子束和可转动四极质谱仪测得产物离子InCl~+、InCl_2~+、PCl~+、PCl_2~+和P_4~+的角分布, 都可用cos~(1.5)θ函数报合. 对于紫外(355 nm)激光诱导反应, 由飞行时间质谱法测得主要产物离子的角分布明显地偏离Knudsen定律. 其中In~+, InCl~+和InCl_2~+的角分布可用α·cosθ+(1-α)cos~nθ函数拟合, 其中α和n为拟合参数, 对于不同的产物离子有不同的数值. 由实验测得的脱附粒子的通量和能量在表面法线方向有明显地聚集现象, 可以认为产物从表面上脱附的机理, 除了热脱附之外, 还有非热脱附以及在表面附近脱附粒子的碰撞效应.     

Molecular Beam Studies on the Laser-Enhanced Surface Reaction of GaAs(100) with Chlorine

A cw supersonic Cl₂ molecular beam coupled with an angle-resolved time-of-flight (TOF) technique has been used to investigate the laser-enhanced surface reaction of GaAs(100) with chlorine. The mass and velocity distributions of the major reaction products under 1064 nm laser irradiation have been measured as a function of laser fluence, detection angle, surface temperature and normal component of the translational energy of the incident chlorine molecules. It has been found that increasing both laser fluence and the translational energy of incident chlorine molecules markedly enhance mis surface reaction. The measured flux angular distributions of major reaction products can be fit satisfactorily with a bi-cosine function. Measurements of the mass and angular distributions of reaction products by a modulated molecular beam mass spectrometry show that the surface temperature effect is obvious for the Cl₂/GaAs(100) “dark” thermal reaction. A direct activated dissociative chemisorption is proposed for the mechanism of Cl₂ chemisorption on the GaAs(100) surface.     

Effect of Laser Pulse Energy on the Characteristics of Cu Nanoparticles Produced by Laser Ablation Method in Acetone

The effect of laser fluence on the characteristics of Cu nanoparticles, prepared by laser ablation method, is investigated experimentally. 1–6 nm Cu nanoparticles were synthesized by the pulsed laser ablation of a high purity copper bulk in acetone. Effect of laser fluence on the size, morphology and structure of produced nanoparticles has been studied. Pulses of a Q-switched Nd:YAG laser of 1,064 nm wavelengths at 7 ns pulse width at different fluences was employed to irradiate the Cu target in acetone. The UV–Vis–NIR absorption spectra of nanoparticles exhibit surface plasmon resonance absorption peak in the visible region. TEM and SEM micrographs indicate that with increasing the laser fluence the average size of spherical Cu nanoparticles is decreased and only the sample which is produced with the highest fluence shows exceptional behavior. It is found that Cu nanoparticles exhibit photoluminescence emission with single peak due to its interband transition.     

角分辨飞行时间法研究GaAs(100)表面蚀刻反应动力学

采用探测室可转动的分子束实验装置,研究了氯分子束与GaAs(100)表面热反应和紫外激光诱导反应的动力学.结果表明,热反应的主要产物为GaCl~3, 其角分布可用cos^2^.^3θ函数拟合.对于紫外(355nm)激光诱导反应,由角分辨的飞行时间(TOF)法测得主要产物为GaCl等,它们的通量角分布须用双余弦加和公式(c~1cosθ+c~2cos^nθ)拟合,表示产物粒子在表面法线方向明显聚集,而且由TOF 谱求得粒子的动能在表面法线方向最大. 这种明显的聚集现象可以由激光诱导的粒子在表面附近发生碰撞效应来解释     

On the iron oxide neutral cluster distribution in the gas phase. I. Detection through 193 nm multiphoton ionization

Iron oxide (FemOn) neutral clusters are generated in the gas phase through laser ablation of the metal and reaction with various concentrations of O2 in He. The mixture of expansion gas and neutral FemOn cluster species is expanded through a supersonic nozzle into a vacuum system, in which the clusters are ionized by an ArF excimer laser at 193 nm, and the ions are detected and identified in a time-of-flight mass spectrometer. In this report, the experimental parameters that influence the observed cluster distributions, such as ablation laser power, expansion pressure, vacuum system pressure, and 193 nm ArF ionization laser power, are explored. In the second paper in this series, the effect of the ionization laser wavelength (355 nm, 193 nm, 118 nm) on the observed cluster ion distribution is explored. The cluster ion distribution observed employing 193 nm laser ionization, is sensitive to the neutral cluster distribution as evidenced by the change in the observed time-of-flight mass spectra with changes in laser power, growth conditions, and expansion conditions. The thermodynamically stable neutral clusters for saturated O2 growth conditions are suggested to be of the forms FemOm, FemO(m+1), and FemO(m+2); which one of these series of neutral clusters is most stable depends on the size of the cluster. For m < 10, FemOm is the most stable neutral cluster series, for 10 < or = m < or = 20, FemO(m+1) is the most stable neutral cluster series, and for 21 < or = m < = 30, FemO(m+2) is the most stable neutral cluster series. Some neutral cluster fragmentation is clearly present for 193 nm ionization due to multiphoton absorption in both the neutral and ionic cluster species.