266 nm激光光解C2H5SSC2H5产物的激光诱导荧光光谱

有机硫化物是大气主要污染物之一,其在大气中的光解产物还将造成二次污染,除了存在于有机硫化物中, S―S键还存在于胱氨酸等蛋白质中, S―S键的形成和断裂决定该类蛋白质的活性.本工作中,我们研究了用实验室常见的Nd:YAG激光器的四倍频266 nm激光光解C₂H₅SSC₂H₅过程,通过激光诱导荧光(LIF)光谱方法检测乙硫自由基C₂H₅S等光解产物.实验表明266 nm激光主要光解C₂H₅SSC₂H₅的S―S键产生C₂H₅S自由基.本文应用密度泛函理论的Becke3-Lee-Yang-Parr泛函(B3LYP方法)得到C₂H₅SSC₂H₅的S―S键、C―S键和C―C键的解离势能曲线,可知在266 nm光解条件下, C₂H₅SSC₂H₅在基态能够发生S―S键、C―S键解离, C―C键不发生解离.本文采用全活化空间自洽场(CASSCF)方法优化得到态和态的C₂H₅S自由基结构及其跃迁的绝热激发能,以辅助解析实验检测的C₂H₅S自由基的LIF光谱.实验结合理论计算最终得出,本实验266 nm光解条件下, C₂H₅SSC₂H₅主要发生S―S键解离,不排除少量分子发生C―S键解离的可能性.     

氧负离子自由基与乙烯反应机理的计算研究

在G3MP2B3理论水平下研究了氧负离子自由基(O^－)与乙烯(C₂H₄)的反应机理. 计算结果表明, O^－与C₂H₄经碰撞快速复合形成离子诱导偶极络合物中间体, 然后经历异构化、解离生成各种产物, 分别对应分子离子异构解离与复合电子剥离反应通道. 通过比较各个反应途径上势垒的相对高度, 发现主要产物通道为复合电子剥离通道, 相应的中性产物主要为c-C₂H₄O; 而分子离子解离通道的通道分支比较小, 其中生成水反应通道相应的阴离子产物主要是CH₂＝C^－. 当前的计算证实了以往实验观察的结论.     

Au(111)面上噻吩加氢脱硫反应机理的理论研究

采用密度泛函理论方法研究了噻吩在Au(111)面上的吸附模式, 并探讨了其在Au(111)面上可能的加氢脱硫反应机理, 对不同机理下各个基元反应的过渡态进行了筛选, 得到了各个步骤的能量变化及所需活化能.计算结果表明, 噻吩在Au(111)面上以S端倾斜吸附在Top位时最稳定.直接脱硫机理表明, 其所需活化能较低, 升高温度有利于提高脱硫反应产率, 但脱硫产物较难控制; 间接脱硫机理表明, 脱硫反应最可能按照加氢异构方式进行, 降低温度有利于脱硫反应产率的提高.随着反应的进行, 噻吩环中的C—S键键长逐渐增大, 键能逐渐减小, 有利于C—S键断裂, 具体步骤为:(1) C₄H₄S+H₂α,α-C₄H₆S; (2) α,α-C₄H₆S+H₂C₄H₈S; (3) C₄H₈S+H₂C₄H₁₀+S, 其中S原子的脱去步骤所需活化能最高, 为反应的限速步骤.     

氟氯酰与丙烷反应的密度泛函理论研究

应用密度泛函理论(DFT), 对氟氯酰(ClF₃O)引发丙烷(C₃H₈)反应生成C₃H₇自由基或丙醇等产物的机理进行了研究. 在B3PW91/6-311＋＋G(d,p)水平上优化了9个不同反应通道上各驻点物(反应物、中间体、过渡态和产物)的几何构型, 并计算了它们的振动频率和零点振动能. 通过零点能校正计算了各反应路径的活化能, 并应用过渡态理论计算了各反应路径常温下的速率常数k. 计算结果表明: ClF₃O与C₃H₈反应可经过不同路径生成HF, C₃H₇自由基和C1F₂O自由基或C₃H₇OH和ClF₃. 其中, 最可几反应路径为ClF₃O分子的中间位F原子进攻丙烷β位H原子的反应, 活化能仅为7.54 kJ/mol, 速率常数为0.153×10⁶ mol^－1•dm³•s^－1.     

乙炔基自由基C2H与氧气反应的密度泛函理论研究

应用量子化学从头算和密度泛函理论(DFT)对C₂H自由基和O₂的反应进行了研究.在B3LYP/6-311G^**水平上优化了反应通道上各驻点(反应物、中间体、过渡态和产物)的几何构型,并计算出它们的振动频率和零点振动能(ZPVE).各物种的总能量由CCSD(T)/6-311G^**//B3LYP/6-311G^**给出,并对能量进行了零点能校正.计算结果表明,反应物中自由基C₂H中的边端C进攻O₂形成了中间体1 (HCCOO),中间体1是一个加合产物.由中间体1经过不同的反应通道可以生成不同的产物P₁ (HCO+CO), P₂ (HCCO+O), P₃(CO₂+CH), P₄ (C₂O+OH)和P₅ (2CO+H).反应通道之间存在着竞争机制.其中P₁, P₂是主要产物,其次还有一定比例的P5生成,而产物P₃, P₄的生成几率较低.各条反应通道化学反应热的计算与实验吻合较好.     

Ar+和trans-/cis-C2H2Cl2解离电荷转移反应的离子速度成像研究(英文)

本文利用离子速度成像方法研究了Ar⁺和trans-/cis-C₂H₂Cl₂的解离电荷转移反应,根据产物离子影像明确了三个反应通道的解离机制.其中,脱氯碎片离子C₂H₂Cl⁺是主要产物,大多数分布在靶分子附近,表明解离过程主要是在大碰撞参数下通过能量共振的电荷转移后发生;同时,有少量的C₂H₂Cl⁺分布在质心附近,这是由C₂H₂Cl₂和Ar⁺在小碰撞参数下发生的紧密碰撞导致的.次要产物C₂HCl⁺展现出与C₂H₂Cl⁺相似的速度分布.而截面最低的产物C₂HCl₂⁺经历了大碰撞参数下的能量共振电荷转移后快速脱氢,基...     

激光诱导的亚硝酸与二苯醚的反应机理

355 nm光照下利用瞬态吸收光谱技术进行了有氧、无氧条件下二苯醚与亚硝酸体系的反应机理研究, 考察了其中瞬态物种的衰减行为, 并对其光解产物进行了GC-MS分析. 研究表明, HNO₂在355 nm紫外光的照射下产生的OH自由基和二苯醚反应生成C₁₂H₁₀O-OH 加合物, N₂条件下C₁₂H₁₀O-OH衰减的速率常数为(1.86±0.14)×10⁵ s^－1, 在有氧条件下, C₁₂H₁₀O-OH可转化为C₁₂H₁₀O-OHO₂, 衰减的速率常数为(6.6±0.4)×10⁶ s^－1. N₂条件下最终产物为苯酚、2-羟基二苯醚、4-羟基二苯醚、4-硝基二苯醚.     

C4H6O,C4H6S与XF (X＝F,Cl, Br)分子间卤键的电子密度拓扑研究

运用MP2/aug-cc-pVDZ方法对2,5-二氢呋喃, 2,5-二氢噻吩与XF (X＝F, Cl, Br)之间的卤键作用进行了理论研究. 研究发现: C₄H₆O, C₄H₆S与XF之间不仅存在O(S)…XF n型卤键, C＝C双键与XF分子亦可形成π型卤键|对于C₄H₆O与XF之间的n型和π型卤键以及C₄H₆S与XF之间的π型卤键, 卤键键能ΔE、键鞍点处的电子密度ρ(r_c)以及电子给体到受体之间的电子转移数Δq(XF)均按B…F₂＜B…ClF＜B…BrF (B＝C₄H₆O, C₄H₆S)的顺序依次增大|对于卤键键能较大的体系C₄H₆O…BrF(n), C₄H₆O…BrF(π), C₄H₆S…F₂(n), C₄H₆S…ClF(n), C₄H₆S…BrF(n), C₄H₆S…BrF(π), 卤键作用介于离子键和共价键之间|而对于其它的卤键键能较小的体系, 卤键作用为闭壳层静电作用.     

有机磷杀虫剂的研究——Ⅶ.某些苯基对位取代硫代膦酸酯的合成

1.制备一些新型的硫代膦酰氯,其中R'为C₆H₅,R"为C₂H₅O,C₂H₅,(CH₃)₂N,(C₂H₅)₂N,C₂H₅S等。     

直链小碳簇Cn(n=3～6)微正则解离速率常数的RRKM理论计算(Ⅰ)

用从头计算法研究小碳簇的解离通道及其动力学.以MP2/6-31G^*精度优化直链C₃,C₄,C₅,C₆及其过渡态的结构,并对它们进行振动分析.在此基础上计算了各解离通道的能垒,并根据RRKM理论估算各个通道的微正则解离速率.计算结果表明,这些小碳簇的解离主要表现为均裂方式.     

Quantum-Chemical Study of Alkyl Carbenium Ions in 100% Sulfuric Acid

A quantum-chemical study of neutral and protonated monoalkyl sulfates RHSO₄and [RH₂SO₄]⁺(where R = CH₃, C₂H₅, iso-C₃H₇, and tert-C₄H₉) is carried out. Calculations are performed using the Hartree–Fock method in the 6-31G** and 6-31++G** basis sets taking into account electron correlation according to the Müller–Plesset perturbation theory MP2/6-31+G*//6-31+G*. Protonated tert-butyl sulfate was also calculated by the DFT B3LYP/6-31++G** method. It was found that monoalkyl sulfates are covalent compounds, and the complete abstraction of alkyl carbenium ions from them has substantial energy cost: 196.4, 161.7, 150.8 and 136.0 kcal/mol, respectively. Protonated methyl and ethyl sulfates are also covalent compounds according to the calculation. They have lower but still high energies of heterolytic dissociation (65.0 and 33.5 kcal/mol, respectively). The energy of R⁺abstraction from protonated isopropyl sulfate is much lower: 23.6 kcal/mol. The main covalent state and the ion–molecular pair, which is a carbenium ion [C(CH₃)₂H]⁺solvated by the H₂SO₄molecule, have about the same energy. The ground state of protonated tert-butyl sulfate corresponds to the ion–molecular complex [C(CH₃)⁺ ₃H₂SO₄] with still lower energy of carbenium ion [C(CH₃)₃]⁺abstraction, which is equal to 10.0 kcal/mol. Calculation according to the DFT B3LYP/6-31++G** method shows the absence of a minimum for the protonated tert-butyl sulfate with a covalent structure on the potential energy surface.     

Conformational study of the structure of free 12-thiacrown-4 and some of its cation metal complexes

Conformational search of 12-thiacrown-4, 12t4, was performed using the CONFLEX method and the MMFF94S force field whereby 156 conformations were predicted. Optimized geometries of the 156 predicted conformations were calculated at the HF, B3LYP, CAM-B3LYP, M06, M06L, M062x and M06HF levels using the 6-311G** basis set. The correlation energy was recovered at the MP2 level using the same 6-311G** basis set. Optimized geometries at the MP2/6-311G** level and G3MP2 energies were calculated for some of the low energy conformations. The D ₄ conformation was predicted to be the ground state conformation at all levels of theory considered in this work. Comparison between the dihedral angles of the predicted conformations indicated that for the stability of 12t4, a SCCS dihedral angle of 180° requirement is more important than a gauche CSCC dihedral angle requirement. Conformational search was performed also for the 12t4?CAg⁺, Bi³⁺, Cd²⁺, Cu⁺ and Sb³⁺ cation metal complexes using the CONFLEX method and the CAChe-augmented MM3 and MMFF94S force fields. Conformations with relative energies less than 10?kcal/mol at the MP2/6-31+G*//HF/6-31+G* level, with double zeta quality basis set on the metal cations, were considered for computations at the same levels as those used for free 12t4, using also the 6-311G** basis set. The cc-pVTZ-pp basis set was used for the metal cations. The predicted ground state conformations of the 12t4?CAg⁺, Bi³⁺, Cd²⁺, Cu⁺ and Sb³⁺ cation metal complexes are the C ₄, C ₄, C ₄, C _2v and C ₄ conformations, respectively. This is in agreement with the experimental X-ray data for the 12t4?CAg⁺ and Cd²⁺ cation metal complexes, but experimentally by X-ray, the 12t4?CBi³⁺ and Cu⁺ cation metal complexes have C _s and C ₄ structures, respectively.     

Density functional B3LYP and B3PW91 studies of the properties of four cyclic organodiboranes with tetramethylene fragments

Molecular structure and vibrational spectra of 1,2-tetramethylenediborane (B₂C₄H₁₂), 1,2:1,2-bis(tetramethylene)diborane (B₂C₈H₁₈), 1,1-tetramethylenediborane (B₂C₄H₁₂) and 1,1:2,2-bis(tetramethylene)diborane (B₂C₈H₁₈), have been studied using quantum computational density functional B3LYP and B3PW91 methods and 6-31G*, 6-31G** and 6-31++G** basis sets. Natural bond orbital analyses have been carried out to study in detail the nature of the B—C, C—C and B—H bonds in these molecules. This study showed that all these compounds are thermodynamically stable in the gas phase, but bicyclic structures are more stable than monocyclic structures.     

Ab Initio calculations on the isomerization of the dimethylene cyclobutene and 1,2,4,5-hexatetraene radical cations to the benzene structure

Ab initio calculations at the MRCI//ROHF/6-31G** level suggest that stable C₆H₆ radical cations formed from dimethylene cyclobutene and 1,2,4,5-hexatetraene either retain the structure of the parent neutral molecule or isomerize to the benzene structure. The previous suggestion from photodissociation experiments that part of the ions from dimethylene cyclobutene isomerize to the 1,2,4,5-hexatetraene structure is not supported by the present results.     

Molecular structure and vibrational spectra of phenobaraitone by density functional theory and ab initio hartree-Fock calculations

Quantum chemistry calculations have been performed using Gaussian03 program to compute optimized geometry, harmonic vibrational frequency along with intensities in IR and Raman spectra at RHF/6-31++G** and B3LYP/6-31++G** levels for phenobarbitone (C₁₂H₁₂N₂O₃) in the ground state. The scaled harmonic vibrational frequencies have been compared with experimental FT-IR and FT-Raman spectra. Theoretical vibrational spectra of the title compound were interpreted by means of potential energy distributions (PEDs) using MOLVIB program. A detailed interpretation of the infrared spectra of the title compound is reported. On the basis of the agreement between the calculated and observed results, the assignments of fundamental vibrational modes of phenobarbitone were examined and some assignments were proposed. The theoretical spectrograms for FT-IR and FT-Raman spectra of the title compound have been constructed.     

Molecular structures and electronic properties of helical thiophene carbon–sulfur oligomers, H2(C2S)nC2H2 (n?=?1–20)

Structure optimizations of the thiophene carbon–sulfur H₂(C₂S) _n C₂H₂ (n = 1–20) were carried out using density functional theory calculations at the B3LYP/6-31G(d) level. The B3LYP/6-31G(d) geometrical data for heptamer H₂(C₂S)₇C₂H₂ and undecamer H₂(C₂S)₁₁C₂H₂ are in good agreement with the X-ray crystallographic data for the helical (C₂S)_n β-heptathiophene and β-undecathiophene, respectively. Structural and electronic properties of helical oligothiophenes obtained at the B3LYP/6-311++G(d,p)//B3LYP/6-31G(d) level are reported. The strain energy formula of n oligothiophenes as a linear function of their molecular length was obtained.     

PCM study of the solvent and substituent effects on bond dissociation energies of the C?NO bond

Quantum chemical calculations are used to estimate the equilibrium C? NO bond dissociation energies (BDEs) for eight X? NO molecule (X = CCl₃, C₆F₅, CH₃, CH₃CH₂, iC₃H₇, tC₄H₉, CH₂CHCH₂, and C₆H₅CH₂). These compounds are studied by employing the hybrid density functional theory (B3LYP, B3PW91, B3P86) methods together with 6‐31G** and 6‐311G** basis sets and the complete basis set (CBS‐QB3) method. The obtained results are compared with the available experimental results. It is demonstrated that B3P86/6‐31G** and CBS‐QB3 methods are accurate for computing the reliable BDEs for the X? NO molecule. Considering the inevitably computational cost of CBS‐QB3 method and the reliability of the B3P86 calculations, B3P86 method with 6‐31G** basis set may be more suitable to calculate the BDEs of the C? NO bond. The solvent effects on the BDEs of the C? NO bond are analyzed and it is shown that the C? NO BDEs in a vacuum computed by using B3PW91/6‐311G** method are the closest to the computed values in acetontrile and the average solvent effect is 1.48 kcal/mol. Subsequently, the substituent effects of the BDEs of the C? NO bond are further analyzed and it is found that electron denoting group stabilizes the radical and as a result BDE decreases; whereas electron withdrawing group stabilizes the group state of the molecule and thus increases the BDE from the parent molecule. © 2009 Wiley Periodicals, Inc. Int J Quantum Chem, 2009     

Dissociative Photoionization of 1,4-Dioxane with Tunable VUV Synchrotron Radiation

The photoionization and photodissociation of 1,4-dioxane have been investigated with a reflectron time-of-flight photoionization mass spectrometry and a tunable vacuum ultraviolet synchrotron radiation in the energy region of 8.0-15.5 eV. Parent ion and fragment ions at m/z 88, 87, 58, 57, 45, 44, 43, 41, 31, 30, 29, 28 and 15 are detected under supersonic conditions. The ionization energy of DX as well as the appearance energies of its fragment ions C₄H₇O₂⁺, C₃H₆O⁺, C₃H₅O⁺, C₂H₅O⁺, C₂H₄O⁺, C₂H₃O⁺, C₃H₅⁺, CH₃O⁺, C₂H₆⁺, C₂H₅⁺/CHO⁺, C₂H₄⁺ and CH₃⁺ was determined from their photoionization efficiency curves. The optimized structures for the neutrals, cations, transition states and intermediates related to photodissociation of DX are characterized at the B3LYP/6-31+G(d,p) level and their energies are obtained by G3B3 method. Possible dissociative channels of the DX are proposed based on comparison of experimental AE values and theoretical predicted ones. Intramolecular hydrogen migrations are found to be the dominant processes in most of the fragmentation pathways of 1,4-dioxane.     

Structural and spectroscopic studies on 2-pyranones

Experimental methods of infrared, Raman and electronic absorption spectroscopy and DFT calculations using B3LYP functionals and 6-31G** and 6-311++G** basis sets have been used to understand the structural and spectral characteristics of 2-pyranones, 6-phenyl-4-methylsulfanyl-2-oxo-2H-pyran and 6-phenyl-4-methylsulfanyl-2-oxo-2H-pyran-3-carbonitrile in the electronic ground (S₀) and first excited (S₁) states. Information about the size, shape, charge density distribution and site of chemical reactivity of the molecules has been obtained by mapping electron density isosurface with electrostatic potential surfaces (ESP). Based on TD-DFT calculations using 6-31+G**5D basis set, an assignment of absorption peaks in the UV–VIS region has been suggested. The S₁ state is found to be a ¹(π,π*) state. A complete vibrational analysis has been attempted on the basis of experimental infrared and Raman spectra and calculated frequency and intensity of the vibrational bands and potential energy distribution over the internal coordinates. Characteristic vibrational bands of the 2-pyranone ring and methylsulfanyl and carbonyl groups have been identified.     

Ab initio study of possible intermediates in the no(4Π) catalyzed geometric isomerizations of olefins

The geometries of acyclic and three-membered ring (nitroxide) H₄C₂NO radicals in their ground ²Π electronic states have been optimized completely at ab initio UHF and ROHF theoretical levels with the STO-3G and the 6-31G** basis sets. The optimizations favour the cyclic nitroxide structure energetically. However ΔE(acyclic - cyclic) at the UHF and ROHF/6-31G** levels are only 3.2 and 1.9 kcal mol^-1, respectively. Incomplete MP2/6-311G** optimizations support these results. The zero-point energy computed at the ROHF/6-31G** level for the nitroxide radical is 2.5 kcal mol^-1 higher than that for the acyclic structure, thus reversing the relative energies by 0.6 kcal mol^-1. The energies of the two radical structures, relative to the sum of those for ethylene and NO, are very close to literature values of the activation energies for the thermal, NO catalyzed geometrical isomerizations of olefins. Thus cyclic nitroxide intermediates may play a role not only in the Hg 6(³P₁) photosensitized, but also in the thermal, NO-catalyzed geometric isomerizations of olefins. Paper dedicated to Professor Otto P. Strausz; presented in part at the 75th Canadian Chemical Congress and Exhibition, Edmonton, May 31 – June 4, 1992.