取代基位置对轮烯衍生物-阶超极化率影响的理论研究

以[12]轮烯为母体,通过改变取代基的位置构造了一系列轮烯衍生物,运用密度泛函B3YLP方法在6-31G(d)基组水平上计算了分子一阶超极化率β和紫外吸收光谱,研究了分子结构和非线性光学性能的关系.研究发现,二维电荷转移(2DCT)分子2～5均具有较大的β值,且分子3的紫外吸收光谱最大吸收峰和其余分子相比发生蓝移,这对解决"非线性效率-透光性矛盾"给予了很大启示.分子2～5的一阶超极化率的大小和分子构型关系密切,随着键长交替(BLA)的增加,分子的β值不断减小.     

取代基位置对轮烯衍生物一阶超极化率影响的理论研究

以 [12]轮烯为母体,通过改变取代基的位置构造了一系列轮烯衍生物,运用密度泛函B3YLP方法在6-31G(d)基组水平上计算了分子一阶超极化率β和紫外吸收光谱,研究了分子结构和非线性光学性能的关系. 研究发现,二维电荷转移（2DCT）分子2-5均具有较大的β值,且分子3的紫外吸收光谱最大吸收峰和其余分子相比发生蓝移,这对解决“非线性效率-透光性矛盾”给予了很大启示. 分子2-5的一阶超极化率的大小和分子构型关系密切,随着键长交替(BLA)的增加,分子的β值不断减小.     

分子一阶超极化率溶剂效应的理论研究

基于一维谐振子模型建立了极性溶剂对光学二阶非线性分子一阶超极化率产生影响的简化理论模型,推导出了非线性分子的线性极化率α和一阶超极化率β的表达式. 以对硝基苯胺为例,所建立的理论模型计算结果较好地解释了实验获得的溶剂极性对其分子线性吸收峰波长（λ_p）和β值的影响. 关键词： 二阶非线性 溶剂效应 谐振子     

轮烯衍生物电子结构及三阶非线性光学性质的理论研究

苯轮烯衍生物具有良好的非线性光学性质. 运用密度泛函理论在不同理论水平和不同基组下计算了轮烯衍生物的静态极化率α和静态第二超极化率γ. 采用含时密度泛函TD-B3LYP方法计算了轮烯分子的紫外吸收光谱. 结果发现: 弥散函数对静态线性极化率α和第二超极化率γ 的计算结果都有显著的影响; 共轭体系的大小和引入的推拉电子基团可以调节轮烯衍生物的第二超极化率. 添加推拉电子基团后不仅能得到更高的非线性光学系数, 也能保证有较好的透光性能, 表明轮稀分子兼具有较高的三阶非线性光学响应和在可见光波段具有良好的透光性的特性. 此外, 采用CAM-B3LYP方法计算了分子1-1和分子2-2的动态(超)极化率. 计算结果表明: 在近红外区, 随着入射光频率的增大, α (ω; ω), γ (-ω; ω, 0, 0) 和γ (-2ω; ω, ω, 0) 都随之增大, 出现近共振增强效应; 在远离共振条件下, α (ω; ω), γ (-ω; ω, 0, 0) 和γ (-2ω; ω, ω, 0) 变化平缓.     

溶剂中一、二维电荷转移分子二阶非线性光学性质理论研究

以典型的一、二维电荷转移分子,对硝基苯胺(pNA),1,3-二氨基-4,6-二硝基苯(DADB)分子为例,运用密度泛函理论(DFT)B3LYP和含时耦合微扰(TDHF)方法在6-31+G(d,p)水平上研究了溶剂和入射光频率对目标分子的非线性光学性质的影响.研究发现溶剂分子对分子一阶超极化率β和紫外吸收光谱的影响很大,但对一阶超极化率各向异性比η和退偏比D的影响很小,这是由于随着溶剂相对介电常数的增加,一阶超极化率的分量︱βxxy︱和︱βyyy︱不断增加,且二者具有很好的线性相关性.然而,考虑色散效应后,不同溶剂中分子的一阶超极化率及其各向异性参数都不相同,色散效应对分子一阶超极化率及其各向异性性质均有很大影响.考虑溶剂效应和色散效应后得到的计算结果与实验结果符合得较好.     

时间分数阶亚扩散方程的高阶差分方法

提出两差分格式求解时间分数阶亚扩散方程.两个格式都是绝对稳定的,收敛阶均为O(τ^q+h²),其中q(q=2-β或2)与方程解的光滑性有关,β(0 < β < 1)是分数阶导数的阶、τ和h分别是时间和空间方向步长.数值实验验证了理论结果的正确性,并与其他方法进行比较,显示了本文方法的有效性和精确性.     

二维电荷转移分子非线性光学性质的理论研究

运用密度泛函理论B3LYP方法在6-31+G（d,p）水平上计算了11个X型二维电荷转移分子的电荷分布、紫外吸收光谱、第一超极化率.结果表明：在x或y方向延长共轭体系,最大吸收波长 红移,第一超极化率 增大,并且在y方向延长共轭体系,能够较好的优化分子透明性与分子非线性光学性质,获得兼具大 和良好透光性的非线性光学性能好的分子;另外,杂原子N取代芳香环上的C原子的位置和数目对分子非线性光学性质有重要影响.     

有机分子二苯乙烯系列衍生物第一超极化率的理论研究

采用耦合-微扰Hartree-Fock方法(CPHF),计算了二苯乙烯系列衍生物的静态第一超极化率.研究发现,具有离域的共轭体系和电子推拉对结构的分子,有利于发生分子内电荷转移,因而具有大的第一超极化率.进一步研究体系中取代基的位置,给体与受体的数量和得失电子的能力,分子的共面性和对称性对分子第一超极化率的影响,结果表明,有机分子拥有更多数量与更强得失电子能力的给体和受体,最高占据分子轨道(HOMO)和最低未占据分子轨道(LUMO)空间分布的不对称,具有较高的原子共面性和较低的分子中心对称性,都能显著增加 关键词： 二苯乙烯 非线性光学 第一超极化率 空间效应     

基于共掺杂调控C32多极矩的二阶非线性光学响应

基于密度泛函(DFT)理论,采用CAM-B3LYP方法,以C₃₂分子为多极矩构建骨架,设计了两类替位式共掺杂的富勒烯衍生物C₂₈B₂N₂和C₂₈B₂P₂,共16种同分异构体,并对它们的电子性质、线性极化率α和一阶超极化率β进行研究。结果表明,掺杂后分子的HOMO-LUMO能隙变小,C₂₈B₂P₂的α和β值均大于C28B2N2系列。其中偶极分子具有大的β值,八极分子则有较小的β值,筛选出具有优异的二阶非线性光学(NLO)响应特性的结构。含时密度泛函理论(TD-DFT)的结果表明,与C₃₂相比,掺杂后所有结构的吸收光谱的响应范围变宽,最大吸收强度减弱,且最大吸收波长的位置发生红移或蓝移。基于完全态求和(SOS)方法,分别用二能级或三能级公式解释了两类共掺杂结构中β值最大的来源,并且证明了与之有关的电子激发类型为π→π*激发。     

苦皮藤中两个新的 β-二氢沉香呋喃型化合物的 NMR 数据解析

从南蛇藤属植物苦皮藤中分离出两个新的β-二氢沉香呋喃型化合物：1β,2β,15-三乙酰氧基-8α-(α-甲基)-丁酰氧基-9β-苯甲酰氧基-4α,6α-二羟基-β-二氢沉香呋喃（化合物I）和1β,15-二乙酰氧基-8α-(α-甲基)-丙酰氧基-2β,9β-二苯甲酰氧基-4α,6α-二羟基-β-二氢沉香呋喃（化合物II）．通过核磁共振（NMR，包括¹H NMR、¹³C NMR、DEPT、¹H-¹H COSY、NOESY、HSQC、HMBC）技术对化合物所有的¹H和¹³C NMR信号进行了全归属和详细解析.     

Raman and mid-infrared spectroscopic study of geometrically frustrated hydroxyl cobalt halides at room temperature

Mid-infrared absorption and Raman spectra of the geometrically frustrated material series,hydroxyl cobalt halides β-Co 2 (OH) 3 Cl and β-Co 2 (OH) 3 Br,are first,to the best of our knowledge,measured at room temperature,to study the corresponding relationship between their vibrational spectral properties and crystal microstructures.Through the comparative analysis of the four spectra we have categorically assigned the OH-related vibration modes of hydroxyl groups in the trimeric hydrogen bond environment (Co 3 ≡OH) 3… Cl/Br,and tentatively suggested vibration modes of O-Co-O,Co-O and Cl/Br-Co-Cl/Br units.These results can also become the basis for analysing their low-temperature spectral properties,which can help to understand the underlying physics of their exotic geometric frustration phenomena around phase transition temperatures.     

Studies of the temperature dependence of the phosphorescence spectra and decay rates of aromatic carbonyl molecules in mixed organic crystals

The temperature dependence of the phosphorescence spectra, decay rates and the S ₀ → T ₂(³ nπ*) absorption spectra were studied for aromatic carbonyl molecules in mixed organic crystals. The energy separation, ΔE_T , between the ³ ππ* lowest excited triplet (T ₁) states and the higher ³ π ^* states (T ₂) was estimated for several systems from the temperature dependence of the phosphorescence spectra and decay rates. It was found that the decay rates of the aromatic carbonyl molecules in the mixed crystal systems studied are determined by (1) thermal population to the ³ nπ* states and (2) increased radiationless transition rates at higher temperatures.     

外电场作用下Si_2O分子的激发特性

主要对2种Si2O分子异构体的激发特性进行研究,由计算结果可知,外电场对Si2O分子的激发能,振子强度,跃迁偶极矩及吸收光谱有着显著的影响.无外电场时三角型Si2O(C2v,1A1)分子在可见光区无吸收谱,外电场作用下其在可见光区(407.18—526.93nm)有比较弱的吸收谱.直线型Si-Si-O(C∞v,3Σ-)分子在有无外电场作用时在蓝光和紫光区均有一定的吸收谱,其中比较难得的是在蓝色光区(478.88—488.59nm)呈现较强的吸收谱.     

Can Raman spectroscopy detect cumulenic structures of linear carbon chains?

The molecular and vibrational structures of cumulenic carbon chains are investigated by density functional theory calculations and compared with that of hydrogen‐capped polyynes. The small value of bond length alternation (BLA) along the CC bonds sequence obtained by geometry optimization of uncapped C_n chains and vinyl‐capped carbon chains confirms their cumulenic structure. It is demonstrated that for finite length chains the structural parameters are determined by end effects as far as the Peierls distortion, expected for very long molecules, does not occur. The Raman spectra of such molecules are calculated to verify the possibility of identifying markers of cumulenic chains by means of vibrational spectroscopy. As expected, the longitudinal mode consisting of the BLA oscillation, which is responsible for the strongest Raman transition of polyynes, becomes very weak for cumulenes; this behaviour is rationalized in terms of local polarizability derivatives. However, other longitudinal modes can be observed in the Raman spectra of C_n chains. The wavenumber behaviour and the optical activity of these modes are interpreted on the basis of the phonon dispersion branch of an ideally infinite cumulenic polymer. Raman intensities computed for chains of different lengths allow to conclude that cumulenic molecules could be detected and identified by means of Raman spectroscopy. Copyright © 2009 John Wiley & Sons, Ltd.     

Solvatochromism,Preferential Solvation of 2,3-Bis(Chloromethyl)-1,4-Anthraquinone in Binary Mixtures and the Molecular Recognition Towards <Emphasis Type="Italic">p</Emphasis>-Tert-Butyl-Calix[4]arene

Optical absorption and fluorescence emission spectra of 2,3-bis(chloromethyl)-1,4-anthraquinone (DCMAQ) in single solvents namely, carbon tetrachloride, acetonitrile, chloroform, propan-2-ol and its binary mixtures [carbon tetrachloride/chloroform, chloroform/acetonitrile, chloroform/propan-2-ol] have been investigated. The preferential solvation of DCMAQ in above mixtures has been studied by monitoring the absorption and fluorescence spectra of DCMAQ. The spectral features indicate that DCMAQ is preferentially solvated by CHCl₃ in the above mixtures. This can be elucidated from the local mole fraction, non-linearity in transition energy plot, preferential solvation index (δ _s2) and (f ₂/f ₁) values. Molecular recognition properties of p-tert-butylcalix[4]arene (tBC) to DCMAQ via hydrogen bonding and π–π interaction were sensed successfully on the basis of absorption and fluorescence emission spectroscopies, by which the stoichiometry ratio and the binding constant of the tBC–DCMAQ complex were determined.     

DasK-Röntgenemissionsspektrum des Chlors in freien Molekülen

TheKα andKβ spectra of chlorine in free molecules were studied using a special fluorescence X-ray tube and a high resolving curved crystal spectrograph with photoelectric registration. It was found that the wavelength shifts of ClKα₁ obtained for various gaseous compounds do not show the regularities observed with solid compounds of other 3rd period elements. — TheKβ spectrum consists of discrete lines the most intense of which result from transitions of the lonely pair electrons of the chlorine atoms. The spectra of HCl, Cl₂ and CH₃Cl can be explained using optical and betaspectroscopical data and MO calculations. The general structure of ClKβ of organic compounds seems to be determined by the hybridisation type of the carbon atoms bound to the chlorine atoms. Evidence is found for a contribution of molecular vibrational energy to the energies of the X-ray transitions.     

DFT approach on stability and conductance of nine different polyyne and cumulene molecules

Cumulene molecules are one of the main candidates for the use as molecular wires. Low bond length alternation (BLA) values are one of the main attractive property of cumulene molecules as it leads to high conductivity, whereas stability under normal conditions is the main problem. The study is aimed at achieving stable molecules with low BLA values by forcing cumulene structure in polyynes through substitution. Hence, we considered symmetric LCC molecules of n core carbon atoms (n?=?4–12) with nine different terminal groups substitution such as hydrogen terminated polyynes (H[n]), phenyl terminated polyynes (Ph[n]), pyridine-capped polyynes Py[n], 3, 5-diphenyl pyridyl terminated polyynes (Py*[n]) their hydrogenated forms (H-Py[n] and H-Py*[n]), oxygen substituted phenyl terminated polyynes (O=Ph[n]) and 2, 4, 6-trimethylphenyl capped cumulenes (Mes[n]). The BLA values, transport barrier, excitation energy, reorganisation energy, energy gap and vertical and adiabatic ionisation energy were analysed to find the suitable molecule for molecular wires.     

XAFS spectra from X-ray fluorescence Kβ line using conventional energy-discriminating detector

X-ray fluorescence spectra of copper (Cu) metal, copper monoxide (CuO), and potassium chromate (K₂CrO₄) were recorded as a function of incident X-ray energy near the Cu K-edge and chromium (Cr) K-edge, respectively, using a conventional silicon drift detector. The spectra contained components due to elastic, inelastic, and multiple scattering, in addition to the Kα and Kβ lines. Cu and Cr K-edge X-ray absorption fine structure (XAFS) spectra of Cu, CuO, and K₂CrO₄ were obtained by an intensity analysis of the Kα and Kβ lines. The intensity of the Kβ line for the different incident photon energies was obtained by numerically removing the additional scattering components using the MUSCAT program. These spectra exhibited a jump near the K absorption edges, which reproduced the spectral features obtained in transmission mode for both Cu, CuO, and K₂CrO₄. A chemical shift was also clearly identified in the X-ray absorption near edges structure using the X-ray fluorescence Kβ line. In addition, the Cr K-edge extended XAFS spectrum of K₂CrO₄ was clearly observed using the Cr Kβ fluorescent line. The XAFS measurements on the Kα and Kβ lines are possible, and they carry equally valuable information.     

Structural and optoelectronic properties of amorphous GaN thin films

Amorphous gallium nitride (a-GaN) thin films were deposited on glass substrate by electron beam evaporation technique at room temperature and high vacuum using N ₂ as carrier gas. The structural properties of the films was studied by X-ray diffraction (XRD) and scanning electron microscope (SEM). It was clear from XRD spectra and SEM study that the GaN thin films were amorphous. The absorbance, transmittance and reflectance spectra of these films were measured in the wavelength range of 300–2200 nm. The absorption coefficient spectral analysis in the sharp absorption region revealed a direct band gap of E _g = 3:1 eV. The data analysis allowed the determination of the dispersive optical parameters by calculating the refractive index. The oscillator energy E ₀ and the dispersion energy E _d, which is a measure of the average strength of inter-band optical transition or the oscillator strength, were determined. Electrical conductivity of a-GaN was measured in a different range of temperatures. Then, activation energy of a-GaN thin films was calculated which equalled E _a = 0:434 eV.