4-苯基-2-苯偶氮基-1-硫代-3, 4-二氮唑硫酮-5的谱学研究

4-苯基-2-苯偶氮基-1-硫代-3,4-二氮唑硫酮-5(C14H10N4S2)由双硫腙与二硫化碳发生加成闭环反应时获得。文章采用紫外-可见光谱的跟踪对双硫腙与二硫化碳的反应进行了系统的研究。初步讨论了反应历程,提出该反应的机理是亲核加成;并通过IR谱和NMR谱,对标题化合物的结构进行了表征。     

H3 PAuPh与(H3PAu)2(1,4-C6H4)2光谱性质的密度泛函研究

用密度泛函(DFT)方法优化了配合物H3 PAuPh(a),(H3 Pau)2(1,4-C6 H4)2(b)的基态的几何结构,并用含时密度泛函方法计算了它们的吸收光谱.结果表明配合物a与b的最低能量吸收谱线的波长分别为257.5 nm和307.6nm,皆具有C(2p)→Au(6p)电荷转移参与下的Px(芳环)→px>(芳环)跃迁本质,并伴有Au(5d)→Au(6p)的金属中心电荷转移性质.配合物b是由两个配合物a相连接而成,配合物b的分子轨道也是由配合物a的分子轨道组合而成.由于轨道组合中存在px或Px相互作用,配合物b的最低能量吸收谱线的波长大于配合物a的相应值.     

2,5-二(4-溴甲基苯基)-1,3,4噁二唑分子的光谱

采用密度泛函理论在B3LYP/6-31+G*水平计算研究2,5-二(4-溴甲基苯基)-1,3,4噁二唑分子的结构、光谱、热力学性质.结果显示,优化得到的最稳定结构的三个环构处于同一平面,两个溴原子分别位于平面的上下两侧.气相中最低能量跃迁与最强吸收峰均出现在315 nm,对应HOMO到LUMO的电子跃迁,溶剂作用使其红移4—6 nm.热力学计算表明,标准摩尔焓、标准摩尔热容和标准摩尔熵等热力学性质与温度之间存在很好的二次函数关系.298.15 K,2,5-二(4-溴甲基苯基)-1,3,4噁二唑分子的标准摩尔生成焓和标准摩尔生成自由能分别为2708.95和2972.13 kJ/mol.     

2,5-二(4-溴甲基苯基)-1,3,4噁二唑分子的光谱

采用密度泛函理论在B3LYP/6-31+G*水平计算研究2,5-二(4-溴甲基苯基)-1,3,4噁二唑分子的结构、光谱、热力学性质.结果显示,优化得到的最稳定结构的三个环构处于同一平面,两个溴原子分别位于平面的上下两侧.气相中最低能量跃迁与最强吸收峰均出现在315 nm,对应HOMO到LUMO的电子跃迁,溶剂作用使其红移4—6 nm.热力学计算表明,标准摩尔焓、标准摩尔热容和标准摩尔熵等热力学性质与温度之间存在很好的二次函数关系.298.15 K,2,5-二(4-溴甲基苯基)-1,3,4噁二唑分子的标准摩尔生成焓和标准摩尔生成自由能分别为2708.95和2972.13 kJ/mol.     

2,5-二(4-溴甲基苯基)-1,3,4噁二唑分子的结构、光谱与热力学性质的理论研究

采用密度泛函理论在B3LYP/6-31+G*水平计算研究2,5-二(4-溴甲基苯基)-1,3,4噁二唑分子的结构、光谱、热力学性质.结果显示,优化得到的最稳定结构的三个环同在一个平面,两个溴原子偏离平面120°,分别位于平面两端正反方向.气相中最强吸收峰出现在315 nm,为S0到S1的电子跃迁,溶剂作用使其红移4～6 nm.热力学计算表明,标准摩尔焓、标准摩尔热容和标准摩尔熵分别与温度存在二次函数关系.298.15 K,2,5-二(4-溴甲基苯基)-1,3,4噁二唑分子的标准摩尔生成焓和标准摩尔生成自由能分别为2708.95和2972.13kJ.mol-1.     

光谱法研究1,3-硫杂杯[4]罗丹明乙二胺酰胺衍生物对Fe3+的探针性能

利用硫杂杯[4]芳烃衍生物与罗丹明乙二胺发生酰化反应,合成了2个具有双罗丹明基团的1,3-硫杂杯[4]罗丹明乙二胺酰胺衍生物.在实验条件下,衍生物与Fe3+均能形成1:1配合物,配合物的形成诱导了衍生物分子中罗丹明基螺环开环,而表现出良好的荧光和比色探针性能.1,3-硫杂杯[4]罗丹明酰胺-2,4-酯对Fe3+的选择性...     

5-羟基-7,4′-二甲氧基二氢黄酮分子结构的理论计算研究

分别应用HartreeFock从头算方法和B3LYP密度泛函方法从黑沙蒿中分离得到的5羟基7,4′二甲氧基二氢黄酮分子的几何构型进行优化,并采用规范不变原子轨道GIAO法,进行核磁共振化学位移计算,得到其两种构型的结构参数和NMR化学位移值,并对理论计算值与实验值的误差进行了统计分析.由计算结果推测该化合物分子结构中C(2)上的H在β位,即C(2)的绝对构型为S型.     

小分子硫原子团簇正离子的结构稳定性

用分子图形软件设计出 4 9种硫原子团簇Sn+ (n =3～ 13)的结构 ,使用B3LYP密度泛函进行几何构型优化和振动频率计算 ,根据分子的总能量得出最稳定的同分异构体 .在硫原子团簇正离子中 ,大部分原子为二配位成键 .带有一、三配位的原子结构的总能量较高 .部分最稳定硫原子团簇正离子的构型与最稳定的中性硫原子团簇的构型完全不同 .     

5-羟基-7,4′-二甲氧基二氢黄酮分子结构的理论计算研究

分别应用Hartree—Fock从头算方法和B3LYP密度泛函方法从黑沙蒿中分离得到的5-羟基-7，4’-二甲氧基二氢黄酮分子的几何构型进行优化，并采用规范不变原子轨道GIAO法，进行核磁共振化学位移计算，得到其两种构型的结构参数和NMR化学位移值。并对理论计算值与实验值的误差进行了统计分析、由计算结果推测该化合物分子结构中C（2）上的H在B位，即C（2）的绝对构型为S型．     

二苯二硫和二苄二硫润滑性能的量子化学研究

用Gaussian03W程序在B3LYP/631G和HF/631G水平上对二苯二硫(DPDS)和二苄二硫(DBDS)的分子几何构型、电子结构、分子轨道指数及与铁原子簇的相互作用等进行了理论计算.用前线分子轨道理论分析了反应的活性原子和活性键,讨论了DPDS和DBDS与铁原子的作用方式,用前线电子密度,超离域性指数,原子净电荷及化合物与铁原子簇的化学吸附作用能等参数作为判据分析了DPDS和DBDS与铁原子间键合的强弱,反应性的大小.计算结果表明DPDS和DBDS与铁接触时,趋向于S-S键与C-S键断裂,在较为缓和的摩擦条件下,DPDS的抗磨作用优于DBDS,在较为苛刻的摩擦条件下,DBDS的极压作用优于DPDS,与摩擦学试验结果一致.     

Nonlinear optical properties of [（CH3）4N]Au（dmit）2 using Z-scan technique

The third-order optical nonlinearities of [（CH3）4N]Au（dmit）2 （dmit = 4,5-dithiolate-1,3-dithiole-2-thione） at 532 nm and 1064 nm are investigated using the Z-scan technique with pulses of picoseconds duration. The Z-scan spectra reveal a strong nonlinear absorption （reverse saturable absorption） and a negative nonlinear refraction at 532 nm. No nonlinear absorption is observed at 1064 nm. The molecular second-order hyperpolarizability γ for the [（CH3）4N]Au（dmit）2 molecule at 532nm is estimated to be as high as （2.1 ±0.1） × 10^-31 esu, which is nearly three times larger than that at 1064 nm. The mechanism responsible for the difference between the results is analysed. Nonlinear transmission measurements suggest that this material has potential applications in optical limiting.     

A theoretical study of the mechanisms for 1,3‐dipolar cycloadditions of diphenyldiazomethane to C60 and C70

The 1,3‐dipolar cycloaddition (1,3‐DPCA) reaction plays a crucial role during the functionalization of fullerenes, which have broad applications in the materials and pharmaceutical fields. In concert with previous experiments, we theoretically investigated the mechanisms of 1,3‐DPCA of diphenyldiazomethane (DDMf) to two fullerenes (C₆₀ and C₇₀) using the M06‐2X density functional method under vacuum and in solvents. To understand the influence of the dipolarophile on these reactions, the 1,3‐DPCA of DDMf to three common acceptors, specifically tetracyanoethylene (TCNE), 2,3‐dichloro‐5,6‐dicyano‐1,4‐benzoquinone (DDQ), and chloranil (CA), was also studied at the same computational level. The substituent effects on the five reactions were investigated by modeling 1,3‐DPCA reactions with 12 different substituted DDMf (DDMs) with five dipolarophiles, totaling 60 reactions. Including the five unsubstituted DDMf reactions, 65 1,3‐DPCA reactions were studied. The stereoselectivity, relative reactivity, solvent effects, and distortion/interaction energy model were carefully considered and analyzed based on their corresponding electronic structures, electrostatic potential surfaces, interaction models, solvent models, and thermodynamic data. An intermediate was identified for each of the 65 reactions. A possible biradical pathway for the reactions between DDMf and the two fullerenes was also investigated. The calculated results corroborate and enrich the experimental observations. The conclusion and detailed discussion are generally important for understanding the 1,3‐DPCA reactions to fullerenes. Copyright © 2014 John Wiley & Sons, Ltd.     

Rectifying effect of heterojunctions between metals and doped conducting polymer nanostructure pellets

This paper reports that the Schottky junctions between low work function metals （e.g. Al and In） and doped semiconducting polymer pellets （e.g. polyaniline （PANI） microsphere pellet and polypyrrole （PPy） nanotube pellet） have been prepared and studied. Since Ag is a high work function metal which can make an ohmic contact with polymer, silver paste was used to fabricate the electrodes. The Al/PANI/Ag heterojunction shows an obvious rectifying effect as shown in I - V characteristic curves （rectifying ratio γ = 5 at ±6 V bias at room temperature）. As compared to the Al/PANI/Ag, the heterojunction between In and PANI （In/PANI/Ag） exhibits a lower rectifying ratio γ= 1.6 at ±2 V bias at room temperature. In addition, rectifying effect was also observed in the heterojunctions Al/PPy/Ag （γ = 3.2 at ±1.6 V bias） and In/PPy/Ag （γ = 1.2 at ±3.0 V bias）. The results were discussed in terms of thermoionic emission theory.     

Synthesis and photoluminescence property of boron carbide nanowires

Large scale, high density boron carbide nanowires have been synthesized by using an improved carbothermal reduction method with B/B203/C powder precursors under an argon flow at 1100℃. The boron carbide nanowires are 5-10 μm in length and 80-100 nm in diameter. Transmission electron microscopy （TEM） and selected area electron diffraction （SAED） characterizations show that the boron carbide nanowire has a B4C rhombohedral structure with good crystallization. The Raman spectrum of the as-grown boron carbide nanowires is consistent with that of a B4C structure consisting of B11C icosahedra and C-B-C chains. The room temperature photoluminescence spectrum of the boron carbide nanowires exhibits a visible range of emission centred at 638 nm.     

Judd--Ofelt analysis of spectra and experimental evaluation of laser performance of Tm3+ doped Lu2SiO5 crystal

This paper reports that the Tm^3＋：Lu2SiO5 （Tm：LSO） crystal is grown by Czochralski technique. The roomtemperature absorption spectra of Tm：LSO crystal are measured on a b-cut sample with 4 at.% thulium. According to the obtained Judd-Ofelt intensity parameters Ω2=9.3155×10^-20 cm^2, Ω4=8.4103×10^-20 cm^2, Ω6=1.5908×10^-20 cm^2, the fluorescence lifetime is calculated to be 2.03 ms for ^3F4 → ^3H6 transition, and the integrated emission cross section is 5.81×10^-18 cm^2. Room-temperature laser action near 2μm under diode pumping is experimentally evaluated in Tm：LSO. An optical-optical conversion efficiency of 9.1% and a slope efficiency of 16.2% are obtained with continuouswave maximum output power of 0.67 W. The emission wavelengths of Tm：LSO laser are centred around 2.06μm with spectral bandwidth of -13.6 nm.     

The effects of interstitial oxygen on superconducting electronic phases in strontium and oxygen co-doped La1.937Sr0.063CuO4＋δ

Strontium and oxygen co-doped La1.937Sr0.063CuO4＋δ superconductor with Tc≈ 40K, which is obtained by oxidizing strontium-doped starting ceramic sample La1.937Sr0.063CuO4 in NaC10 solution, is annealed under different conditions to allow interstitial oxygen to redistribute. The evolution of the intrinsic superconducting property with the oxygen redistribution is studied in detail by magnetic measurements in various fields. It is found that there occurs the electronic phase separation from the single superconducting phase with Tc ≈ 40 K into two coexisting superconducting states with values of Tc： 15 and 40K or of 15 and 35 K in this system, depending on annealing condition. Our results indicate that the 15, 35 and 40 K superconducting phases associated with the excess oxygen redistribution are all thermodynamically meta-stable intrinsic states in this Sr/O co-doped cuprate.     

Low-temperature heat capacities and standard molar enthalpy of formation of 4-（2-aminoethyl）-phenol （C8H11NO）

This paper reports that low-temperature heat capacities of 4-（2-aminoethyl）-phenol （C8H11NO） are measured by a precision automated adiabatic calorimeter over the temperature range from 78 to 400 K. A polynomial equation of heat capacities as a function of the temperature was fitted by the least square method. Based on the fitted polynomial, the smoothed heat capacities and thermodynamic functions of the compound relative to the standard reference temperature 298.15K were calculated and tabulated at the interval of 5K. The energy equivalent, εcalor, of the oxygen-bomb combustion calorimeter has been determined from 0.68g of NIST 39i benzoic acid to be εcalor=（14674.69±17.49）J·K^-1. The constant-volume energy of combustion of the compound at T=298.15 K was measured by a precision oxygen-bomb combustion calorimeter to be ΔcU=-（32374.25±12.93）J·g^-1. The standard molar enthalpy of combustion for the compound was calculated to be ΔcHm = -（4445.47 ± 1.77） kJ·mol^-1 according to the definition of enthalpy of combustion and other thermodynamic principles. Finally, the standard molar enthalpy of formation of the compound was derived to be ΔfHm（C8H11NO, s）=-（274.68 ±2.06） kJ·mol^-1, in accordance with Hess law.     

Covalent binding of cyclohexene, 1,3-cyclohexadiene and 1,4-cyclohexadiene on Si(1 1 1)-7 × 7

The adsorption reactions and binding configurations of cyclohexene, 1,3-cyclohexadiene and 1,4-cyclohexadiene on Si(1 1 1)-7 × 7 were studied using high-resolution electron energy loss spectroscopy (HREELS), ultraviolet photoelectron spectroscopy (UPS), X-ray photoelectron spectroscopy (XPS) and DFT calculation. The covalent attachments of these unsaturated hydrocarbons to Si(1 1 1)-7 × 7 through the formation of Si–C linkages are clearly demonstrated by the observation of the Si–C stretching mode at 450–500 cm⁻¹ in their HREELS spectra. For chemisorbed cyclohexene, the involvement of π_C=C in binding is further supported by the absence of C=C stretching modes and the disappearance of the π_C=C photoemission. The chemisorption of both 1,3-cyclohexadiene and 1,4-cyclohexadiene leads to the formation of cyclohexene-like intermediates through di-σ bonding. The existence of one π_C=C bond in their chemisorbed states is confirmed by the observation of the C=C and (sp²)C---H stretching modes and the UPS and XPS results. DFT calculations show that [4 + 2]-like cycloaddition is thermodynamically preferred for 1,3-cyclohexadiene on Si(1 1 1)-7 × 7, but a [2 + 2]-like reaction mechanism is proposed for the covalent attachment of cyclohexene and 1,4-cyclohexadiene.     

The characteristics of O＋HD （v = 0, j = 0） reaction dynamics

The analytical potential energy function of HDO is constructed at first using the many-body expansion method.The reaction dynamics of O+HD(v = 0,j = 0) in five product channels are all studied by quasi-classical trajectory(QCT) method.The results show that the long-lived complex compound HDO is the dominant product at low collision energy.With increasing collision energy,O+HD → OH+D and O+HD → OD+H exchange reactions will occur with remarkable characteristics,such as near threshold energies,different reaction probabilities,and different reaction cross sections,implying the isotopic effect between H and D.With further increasing collision energy(e.g.,up to 502.08 kJ/mol),O+HD → O+H+D will occur and induce the complete dissociation into single O,H,and D atoms.     

单个谐振子波函数中的有效β值

当一个简单谐振子波函数(SHO)作为有效波函数时,在SHO波函数里面一个重要的参数是有效$ \, \beta$值。得到了简单谐振子波函数有效$ \, \beta$值($ \, \beta_{\rm eff}$)在坐标空间和动量空间的解析表达式。将解析式运用到轻介子系统($u\bar{u}, \, u\bar{s}$)比较 $ \, \beta_{\rm eff}$的行为,结果表明在基态时坐标空间的$ \, \beta_ {{\rm eff}, \, \boldsymbol{r}}$和动量空间的$ \, \beta_ {{\rm eff}, \, \boldsymbol{p}}$在康奈尔势下的值不相同,而在高激发态时两者大小相近。