大气汽溶胶微粒子光学特性的研究

根据Mie微粒子光散射理论计算了汽溶胶大气模型的光学特性,得到了汽溶胶的散射截面、吸收截面和消光截面以及红外波段散射强度分布,同时计算了汽溶胶大气的发射率光谱,为研究大气红外传输提供了计算方法。     

胶原接枝改性用于制备红外低发射率涂层的研究

用甲基丙烯酸甲酯在硝酸铈铵和偶氮二异丁腈的联合引发下对胶原进行接枝共聚改性,并用制得的胶原接枝共聚物颗粒与氧化铟纳米粒子复合制成涂层.研究了接枝反应温度及萃取剂对胶原接枝共聚物及其复合物涂层的红外发射率的影响,同时对复合物涂层红外发射率的降低机理进行了初步探讨.结果表明,在反应温度为50～55℃时,先后用丙酮和水作为萃取剂,可制得粒径为40～80nm的胶原接枝共聚物颗粒,该颗粒与氧化铟纳米粒子复合后,涂层的红外发射率(8～14μm)较单一的胶原接枝共聚物和氧化铟纳米粒子的红外发射率明显降低,胶原接枝共聚物纳米颗粒和氧化铟纳米粒子之间显示出较强的复合协同效应.     

基于计算最大差异光谱的目标转换因子分析用于解析混合物红外光谱

基于因子分析的目标转换法[1]利用抽象光谱构成的矩阵具有使纯物种光谱向自身逐步逼近的性质[2],用于混合物红外光谱的解析,简单明确[3]．在进一步的探索中,我们发现该算法对原始光谱的构成具有较强的依赖性．本文特别构造了这样的体系,即在混合物样品中剔除了某一物种占优势的样品,应用新算法后,避免了对采样的依赖性．1方法与原理根据自模拟曲线分辨算法（SelfModelingCurveResolution,SMCR）[4~6],纯物种光谱可写成式中,Akj为抽象正交光谱,Xik为系数,Fij为纯物种光谱,n为物种数．根据吸光度不能为负这一限制条件,可以…     

共聚物红外光谱的小波变换

用傅里叶变换红外光谱研究了辐射合成的丙烯酰胺、丙烯酸钠均聚物水凝胶和几种丙烯酰胺／丙烯酸钠配比不同的共的水凝胶的组成变化，发现共聚物的特征吸收带重叠得比较严重，尤其当丙烯酸单元含量较代时，其特征吸收带大部分则不能分辨，将其红外光谱经波波变换后，这类共聚物的特征吸收带较好地得到分离，成功地提高了红外光谱图的分辨率，有助于更好地定性或定量表征共聚物的组成。     

杂多化合物的红外光谱研究

本文研究了与Ｋｅｇｇｉｎ结构相关的３１种３大系列（２：１８系列，１：１１系列和双系列）杂多化合物的红外光谱，它们是：ＮＰ２Ｗ１８（Ｎ＝（ＣＨ３）４Ｎ＾＋，（Ｃ２Ｈ５）４Ｎ＾＋，（Ｃ４Ｈ９）４Ｎ＾＋），ＭＰ２Ｗ１８（Ｍ＝Ｌｉ＾＋，Ｎａ＾＋，Ａｇ＾＋，Ｃｕ＾２＋）；ＫｎＺＷ１１（Ｚ＝Ｐ，Ｂ，Ｇｅ，Ｓｉ），ＭＳｉＷ１１（Ｍ＝Ｍｎ，Ｚｎ，Ｃｕ，Ｃｏ，Ｎｉ）和Ｍ（ＰＷ１１）２（Ｍ＝Ｃｅ，Ｐｒ，Ｎｄ，Ｓｍ，Ｅ     

LB膜的红外光谱研究方法

LB膜是规则排列的单分子层膜或组合单分子层膜,膜的功能取决于膜的二维有序取向特征。因此,LB膜的表征就成为一个极其重要的课题。红外光谱(IR)是研究分子结构的重要手段之一,用IR方法可以研究LB膜体     

变温傅里叶红外光谱技术研究硬脂酸结构及相变机理

采用傅里叶红外光谱法研究了温度对于硬脂酸分子结构影响。通过变温红外技术在293~393K范围内,分别测定了硬脂酸羰基的傅里叶红外光谱、二阶导数红外光谱及去卷积红外光谱。结果表明,硬脂酸主要存在反式二聚体1、顺式二聚体2、开环二聚体3及单体4等4种结构。     

红外光谱振动模式分解及应用

本文用群论方法推出多原子分子正则振动模式的可约表示特征标公式,在IBM微机上实现程序化,使红外光谱振动模式分解更加简便、实用。并且给出AB_n(n=2～12)构型分子和碳原子簇C_n(n=20,24,50,60,70,84)的振动模式不可约表示。     

液晶聚合物材料的红外光谱表征

红外光谱以高选择性、无破坏性以及高超的分辨和实时跟踪能力成为从分子水平研究液晶聚合物的的重要分析手段,而偏振二向色技术、时间分辨步扫描技术和二维相关分析技术的发展进一步提高了红外光谱分析复杂液晶聚合物的能力。本文介绍了传统傅里叶变换红外光谱及各种新型光谱分析技术（主要是二维相关技术）对液晶聚合物材料表征的研究进展,特别是对于液晶聚合物分子氢键、共聚和共混物相容性以及外场（温度、电场、光场、应力场）作用下液晶分子取向等的研究,并分别进行了具体的应用实例分析。     

Calculation of photoionization differential cross sections using complex Gauss‐type orbitals

Accurate theoretical calculation of photoelectron angular distributions for general molecules is becoming an important tool to image various chemical reactions in real time. We show in this article that not only photoionization total cross sections but also photoelectron angular distributions can be accurately calculated using complex Gauss‐type orbital (cGTO) basis functions. Our method can be easily combined with existing quantum chemistry techniques including electron correlation effects, and applied to various molecules. The so‐called two‐potential formula is applied to represent the transition dipole moment from an initial bound state to a final continuum state in the molecular coordinate frame. The two required continuum functions, the zeroth‐order final continuum state and the first‐order wave function induced by the photon field, have been variationally obtained using the complex basis function method with a mixture of appropriate cGTOs and conventional real Gauss‐type orbitals (GTOs) to represent the continuum orbitals as well as the remaining bound orbitals. The complex orbital exponents of the cGTOs are optimized by fitting to the outgoing Coulomb functions. The efficiency of the current method is demonstrated through the calculations of the asymmetry parameters and molecular‐frame photoelectron angular distributions of and . In the calculations of , the static exchange and random phase approximations are employed, and the dependence of the results on the basis functions is discussed. © 2017 Wiley Periodicals, Inc.     

Absolute photoionization cross sections of two cyclic ketones: cyclopentanone and cyclohexanone

Absolute photoionization cross sections for cyclopentanone and cyclohexanone, as well as partial ionization cross sections for the dissociative ionized fragments, are presented in this investigation. Experiments are performed via a multiplexed photoionization mass spectrometer utilizing vacuum ultraviolet (VUV) synchrotron radiation supplied by the Advanced Light Source of Lawrence Berkeley National Laboratory. These results allow the quantification of these species that is relevant to investigate the kinetics and combustion reactions of potential biofuels. The CBS‐QB3 calculated values for the adiabatic ionization energies agree well with the experimental values, and the identification of possible dissociative fragments is discussed for both systems. Copyright © 2017 John Wiley & Sons, Ltd.     

Investigation on the absolute and relative photoionization cross sections of 3 potential propargylic fuels

Absolute photoionization cross sections for 2 potential propargylic fuels (propargylamine and dipropargyl ether) along with the partial ionization cross sections for their dissociative fragments are measured and presented for the first time via synchrotron photoionization mass spectrometry. The experimental setup consists of a multiplexed orthogonal time‐of‐flight mass spectrometer and is located at the Advanced Light Source facility of the Lawrence Berkeley National Laboratory in Berkeley, California. Data for a third propargylic compound (propargyl alcohol) were taken; however, because of its low signal, due to its weakly bound cation, only the dissociative ionization fragment from the H‐loss channel is observed and presented. Suggested pathways leading to formation of dissociative photoionization fragments along with CBS‐QB3 calculated adiabatic ionization energies and appearance energies for the dissociative fragments are also presented.     

Absolute partial and total electron ionization cross sections for CCl4 from threshold up to 180 eV

Electron impact ionization of carbon tetrachloride was studied as a function of electron energy from threshold up to 180 eV. A double-focusing mass spectrometer system in combination with an improved electron impact ion source was used, alleviating the problems of ion extraction from the source and the transmission of the extracted ions through the mass spectrometer system. Absolute partial ionization cross sections for the occurrence of CCl ₃ ⁺ , CCl ₂ ⁺ , CCl⁺, Cl ₂ ⁺ , Cl⁺, C⁺, CCl ₃ ²⁺ , and CCl ₂ ²⁺ have been determined. In addition, the total ionization cross-section function of CCl₄ is reported and compared with theoretical predictions based on a classical binary encounter approximation. Using nth root extrapolation the following ionization energies of the doubly ionized fragment ions have been derived: AE(CCl ₃ ²⁺ )=30.4±0.3 eV; and AE (CCl ₂ ²⁺ )=31.8±0.3 eV. In accordance with theoretical predictions and previous results, no stable CCl ₄ ⁺ has been detected, however, metastable dissociation processes CCl ₄ ⁺ CCl ₃ ⁺ have been observed.     

Elastic and inelastice-CF3OCF3 cross sections from swarm data

The total vibrationally inelastic and the momentum-transfer elastic e-CF₃0CF₃ cross sections are obtained by the best fit of the measured electron drift velocity in pure CF₃OCF₃ as well as in its mixtures with Ar.     

Calculation of cross sections for positron-Ar collisions

The three-body classical trajectory Monte-Carlo (CTMC) method is used to investigate positron-argon atom collisions. The total ionization cross sections are presented along with singly and doubly differential cross sections. The existence of the cusp-like peak in the triply differential electron and positron spectra at positron impact is predicted.     

Stimulated emission cross sections and temperature-dependent spectral shifts of neutral nitrogen-vacancy centers in diamonds

The neutral nitrogen-vacancy (NV⁰) defects in diamond are photostable color centers, suitable for a wide range of applications in science and engineering. However, the photophysical properties of the centers have not yet been fully characterized. This work measured the stimulated emission cross sections of NV⁰ in a single-crystal diamond by two-photon excitation of its matrix at 344 nm. From the measured photoluminescence spectrum and the fluorescence lifetime of 20 ± 1 ns, we determined a peak stimulated emission cross section of 1.43 ± 0.07 × 10⁻¹⁷ cm² at 650 nm for the NV⁰ centers. In addition, we have also examined the thermal shifts of the zero-phonon line of NV⁰ centers in nanoscale diamonds (~100 nm in diameter) over the temperature range of 30–120°C. A temperature measurement sensitivity of 0.2 K·Hz^−1/2 was achieved, which is about two-fold better than that of NV⁻, despite that the fluorescence intensity of NV⁰ is about six-fold lower than that of NV⁻ in the same nanoparticles. The result is attributed to the smaller electron–phonon coupling strength of the neutral center, compared with its negatively charged counterpart.     

Absolute partial cross sections and kinetic energy analysis for the electron impact ionization of ethylene

We present absolute partial electron impact ionization cross sections for ethylene in the electron energy range between threshold and 1000 eV measured with a two sector field double focusing mass spectrometer. Ion kinetic energy distribution functions have been measured at all electron energies by applying a deflection field method. Multiplication of the measured relative cross sections by the appropriately determined discrimination factors lead to accurate relative partial cross sections. Normalization of the sum of the relative partial cross sections to an absolute total cross section gives absolute partial cross section values. The initial kinetic energy distributions of several fragment ions show the presence of two or more contributions that exhibit different electron energy dependencies. Differential cross sections with respect to the initial kinetic energy of the ions are provided and are related to specific ion production channels. The electron threshold energies for the direct and numerous other dissociative ionization channels are determined by quantum chemical calculation and these allow the determination of the total kinetic energy release and the electron energy loss for the most prominent dissociative ionization channels.     

Photoionization cross sections with optimized orbital exponents within the complex basis function method

We show a new direction to expand the applicability of the complex basis function method for calculating photoionization cross sections through the imaginary part of the frequency-dependent polarizability. Based on the variational stability of the frequency-dependent polarizability, we made nonlinear optimizations of complex orbital exponents in basis functions representing continuum wave functions, and obtained fairly accurate results for H atom with only one or two complex basis functions particularly with dipole velocity gauge. Results were almost independent of whether Slater-type or Gaussian-type orbitals are used, implying the applicability to general many electron problems. The method was also applied to the (1)S (1s)(2) --> (1)P (1s)(1)(kp)(1) cross section of He atom and the optimized complex orbital exponents were related to those of H atom through the scaling property. The nonlinear optimizations have converged smoothly and the cross sections were in excellent agreement with experiment throughout wide photon energies, which suggest the effectiveness of the approach for many-electron systems.