FC(O)O2的结构及其自由基与NO反应的微观机理研究

用密度泛函理论(DFT)和哈特里-福克(HF)从头计算方法和半经验势方法等研究了FC(O)O₂ 的结构和振动性质.在DFT中采用B3LYP方法,在6-311G(d)基组上对FC(O)O₂自由基与NO反应的微观过程进行了分析.首先给出了各反应物、中间体、过渡态和生成物的几何构型,然后计算了它们的能量和频率,通过频谱分析得到反应的中间体和过渡态信息,即FC(O)O₂与NO反应为多反应通道,势垒高度和反应速度给出主要通道是FC(O)O₂     

异硫氰酸与CF2自由基反应机理的量子化学研究

采用密度泛函理论B3LYP方法研究了CF₂自由基与HNCS的反应机理,并在B3LYP/6-311++G**水平上对反应物、中间体、过渡态进行了全几何参数优化,通过频率分析和IRC确定中间体和过渡态的真实性.为了得到更精确的能量值,又用CCSD（T）/6-311++G**方法计算了在B3LYP/6-311++G**水平优化后的各个驻点的相对能量.根据统计热力学及用Winger校正的Eyring过渡态理论,利用自编程序,计算不同温度下低势垒反应的平衡常数和速率常数.计算结果表明,单重态的CF₂自由基与HNCS的反应有6条可能的反应通道,三重态的CF₂自由基与HNCS的反应有1条反应通道.其中单重态反应通道CF₂+HNCS→IM1→TS1→IM2 HCF₂NCS（P1）为主反应通道.     

锗烯与异氰酸多通道反应的理论计算

采用密度泛函理论B3LYP方法研究了单重态GeH₂与HNCO的反应机理.在B3LYP/6-311++G**水平上对反应物、中间体、过渡态进行了全几何参数优化,通过频率分析和内禀反应坐标（IRC）确定中间体和过渡态,用QCISD（T）/6-311++G**方法计算了各个驻点的单点能.计算表明单重态的锗烯与异氰酸的反应有抽提氧、插入N-H键、抽提亚氨基的反应路径.采用经Winger校正的Eyring过渡态理论分别计算了1个大气压、不同温度下反应势垒较低通道的热力学及动力学性质,结果表明插入N-H键反应（GeH₂+HNCO→IM7→TS6→P2）通道在温度400 K～1400 K内,有较高的平衡常数和反应速率常数,为主反应通道,主产物为GeH₃NCO.     

SiH3+O(3P)反应机理的理论研究

利用abinitio方法对SiH3+O(3P)反应进行了理论研究,在MP2/6-311+G(d,p)水平上优化得到了反应途径上的反应物、中间体、过渡态和产物的几何构型,并在QCISD(T)/6-311+G(d,p)水平上进行单点能计算.计算结果表明,SiH3+O(3P)→IM1→TS3→IM2→TS8→HOSi+H2为主反应通道,其他可能存在的次要产物有HSiOH+H、H2SiO+H和HSiO+H2.HOSi、HSiO和HSiOH(cis)还可能进一步解离生成SiO.另外,计算结果对SiH4+O(3P)反应机理中存在的争议给出了可能的解释,认为Withnall等人在实验中观察到的产物HSiOH、H2SiO和SiO并不是SiH4+O(3P)反应的直接产物,而是来自副反应SiH3+O(3P).     

CH2F自由基与HNCO反应机理的理论研究

采用密度泛函理论的B3LYP方法,在6-311 G(d,p)基组水平上研究了CH2F自由基与HNCO的微观反应机理,优化了反应过程中的反应物、中间体、过渡态和产物的几何构型,通过振动分析验证了所有可能的过渡态;并且还在QCISD(T)/6- 311 G**//B3LYP/6-311 G(d,p)机组水平上计算了相应单点能．找到了CH2F自由基与HNCO反应的7条可行的反应通道,对结果的分析表明,CH2F HNCO→TS8→IM5→TS9→IM4通道的控制步骤活化能最低,是该反应的主要通道．     

Cl对气态亚硝酸（HONO）直接提氢反应机理的研究

采用密度泛函理论研究了Cl对气态亚硝酸（HONO）直接提取氢的反应机理。在B3LYP/6-311G(d,p)水平上,优化得到了反应途径上的反应物、中间体、过渡态和产物的几何构型;通过频率分析对各分子构型进行了确认;并利用QCISD(T)方法计算了各分子单点能量。计算结果表明,HONO分子具有顺式和反式两种构型;常温条件下,Cl对顺式构型直接提取氢的反应竞争性具有明显优势,其主要反应途径为：cis-HONO+Cl→cis-M1→cis-TS→cis-M2→HCl+NO2。     

二氯卡宾与异氰酸反应机理的量子化学研究

采用密度泛函理论B3LYP方法研究了CCl2自由基与HNCO的反应机理,并在B3LYP/6-311++G**水平上对反应物,中间体,过渡态进行了全几何参数优化,通过频率分析和IRC确定中间体和过渡态。为了得到更精确的能量值,用QCISD(T)/6-311++G**方法计算了各个驻点的单点能,计算结果表明单重态的二氯卡宾与异氰酸的反应有抽提氧、插入N-H键、抽提亚氨基的路径。而插入通道HNCO + CCl2→IM3 →TS2→P2(C2Cl2ONH) 反应能垒最低, 为主反应通道。     

2-甲基-1,3-顺丁二烯在Rh(Ⅰ)催化下与苯甲醛反应机理的研究北大核心CSCD

采用密度泛函方法(DFT)研究了2-甲基-1,3-顺丁二烯在Rh(Ⅰ)催化下与苯甲醛反应生成高烯丙基醇的反应机理.在B3LYP/6-31+G*水平上优化了反应过程中所有反应物、过渡态、中间体以及产物的几何构型,通过能量和振动分析确认了过渡态的真实性.并且在相同基组水平上应用自然键轨道(NBO)、前线轨道理论和分子中的原子(AIM)理论分析了这些化合物的成键特征和轨道间的相互作用.报道了可能的反应通道IA:Re→IMA1→TSA1→IMA2→IMA3→TSA2→IMA4→IMA5→TSA3→IMA6→PA;IB:Re→IMB1→TSB1→IMB2→IMB3→TSB2→IMB4→IMB5→TSB3→IMB6→PB,根据相对能量分析确定反应通道IB具有相对较低的活化能,是反应的主通道,与实验结果一致.     

2-甲基-1,3-顺丁二烯在Rh(Ⅰ)催化下与苯甲醛反应机理的研究

采用密度泛函方法(DFT)研究了2-甲基-1,3-顺丁二烯在Rh(Ⅰ)催化下与苯甲醛反应生成高烯丙基醇的反应机理.在B3LYP/6-31+G*水平上优化了反应过程中所有反应物、过渡态、中间体以及产物的几何构型,通过能量和振动分析确认了过渡态的真实性.并且在相同基组水平上应用自然键轨道(NBO)、前线轨道理论和分子中的原子(AIM)理论分析了这些化合物的成键特征和轨道间的相互作用.报道了可能的反应通道IA:Re→ IMA1→TSA1→IMA2→ IMA3→ TSA2→IMA4→IMA5→ TSA3→IMA6→PA;IB:Re→IMB1→TSB1→IMB2→IMB3→TSB2→ IMB4→ IMB5→TSB3→ IMB6→ PB,根据相对能量分析确定反应通道IB具有相对较低的活化能,是反应的主通道,与实验结果一致.     

Mg(NH2)2与LiH放氢反应机理的密度泛函理论研究

采用密度泛函理论B3LYP方法研究Mg(NH₂)₂与LiH放氢反应机理,在6-311G(d,p)基组水平上对反应物、中间体、过渡态及产物进行全几何参数优化,频率分析和内禀反应坐标(IRC)计算证实中间体和过渡态的正确性和相互连接关系.计算结果表明,反应分三个阶段,包括第一步氢取代反应,第二步氢取代反应和脱氢后的异构化反应.反应有两条途径,其中第二步对位氢取代反应所对应通道为主反应通道.反应释放的H₂中两个氢原子分别来源于Mg(NH₂)₂和LiH.     

Mechanistic study on Mo(CO)6‐catalyzed intramolecular [2 + 2] or [2 + 2 + 1] cycloaddition reaction of 5‐allenyl‐1‐ynes

By means of density functional theory, the Mo(CO)₆‐catalyzed intramolecular [2 + 2] or [2 + 2 + 1] cycloaddition reaction of 5‐allenyl‐1‐ynes was investigated. All the intermediates and transition states were optimized completely at B3LYP/6‐311++G(d,p) level (LANL2DZ(f) for Mo). Calculations indicate that the complexation of 5‐allenyl‐1‐ynes with Mo(CO)₆ occurred preferentially at the triple bond to give the complex M1 and then the complexation with the distal double bond of the allenes generates the complex M5 . In this reaction, Mo(CO)₆‐catalyzed intramolecular [2 + 2] cycloaddition is more favorable than [2 + 2 + 1] cycloaddition. The reaction pathway Mo(CO)₆ + R → M5 → T7 → M12 → M13 → T11 → M18 → P4 is the most favorable one, and the most dominant product predicted theoretically is P4 . The solvation effect is remarkable, and it decreases the reaction energy barriers. Copyright © 2011 John Wiley & Sons, Ltd.     

Nitric oxide reduction by CO ON Rh(111): Temperature programmed reaction

The reaction of NO with CO on Rh(111) has been studied with temperature programmed reaction (TPR). Comparisons are made with the reaction of O₂ with CO and the reaction of NO with H₂. The rate-determining step for both CO oxidation reactions is CO(a) + O(a) → CO₂(g). Repulsive interactions between adsorbed CO and adsorbed nitrogen atoms lead to desorption of CO in a peak at 415 K which is in the temperature range where the reaction between CO(a) and O(a) produces CO₂(g). Thus the extent of reaction of CO(a) with NO(a) is less than that between CO(a) and O(a) due to the lower coverage of CO caused by adsorbed N atoms and NO. A similar repulsive interaction between NO(a) and H(a) suppresses the NO + H₂ reaction. CO + NO reaction behavior on Rh(111) is compared to that observed on Pt(111).     

Vector correlations of the reaction O(1D) + H2 on the DK potential energy surface

This paper reports on the angular momentum polarization of the products of the reaction O(¹D₂) + H₂ via the quasiclassical trajectory (QCT) calculation on the DK (Dobbyn and Knowles) potential energy surface (PES). The four polarization-dependent differential cross-sections (PDDCS) (0, 0), (2, 0), (2, 2), (2, ?1) were calculated at different collision energies. The vector correlation between reagent velocity and product angular moment, the vector correlation between reagent, product velocity and product angular moment were studied. From the calculations, it can be obtained that the OH products are produced mainly in the plane of H–O–H plane. The changes of OH products angular momentum j ′ direction along with the increasing collision energies were ascribed to the existence of a new reaction mechanism.     

Isomers of OCS and their reaction with H2O on singlet potential energy surface

The isomers of the carbonyl sulfide (OCS) molecule are investigated in detail at CCSD(T)/cc-pVTZ//MP2/6-311++G(2d,2p) level of theory. One cyclic isomer was identified along with three different linear minima of the OCS molecule. Three interconversion transition states were also located between cyclic and linear forms of OCS. Among these four isomers, the singlet potential energy surface (PES) for the molecule–molecule reaction between the three most energetically favoured isomers of OCS and H₂O has been explored theoretically at the CCSD(T)/cc-pVTZ//MP2/6-311++G(2d,2p) level. This singlet PES comprises of three paths. Path 1 is the reaction of linear OCS molecule with water producing the major product P1 (CO₂?+?H₂S), minor product P2 (S?+?HCOOH) and two isomers via 14 minima and 15 transition states. The Path 2 is an isomerization process in which cyclic isomer of OCS reacts with water molecule via another initial barrierless aduct producing five isomers of the OCS–H₂O system through five interconversion transition states. The reaction of linear COS isomer with water is shown in Path 3. This path produces the radicals SH and COOH from another COS–H₂O complex via a transition state. Among these three products, the product P1 is energetically most favoured. The overall exothermicity of the product channels for the formation of major product P1 on PES is calculated to be about 10.60?kcal/mol possessing initial high entrance barriers of 45.48 and 55.47?kcal/mol in two possible pathways. As the process is favoured thermodynamically but not kinetically, the reaction is expected to be very slow.     

Dependence on collision energy of the stereodynamical properties of the 18O + 32O2 exchange reaction

We report a quantum stereodynamical study of the ¹⁸O + ¹⁶O¹⁶O(v = 0, j = 1) → ¹⁸O¹⁶O(v′ = 0, j′) + ¹⁶O oxygen exchange reaction at four different collision energies. We calculated the polarisation moments and generated stereodynamical portraits related to the key vectors involved in this collision process. Ozone complex-forming approaches of reactants are then deduced. The results indicate that different approaches are possible but strongly depend on the collision energy and other parameters of the collision. We also conclude that the reaction globally tends to favour a perpendicular approach with increasing energy.     

Additional information from the measurements by Hushfar,Rogers and Stair of the infrared chemiluminescence from the reaction N+O2 → NO+O

Hushfar et al. measured the chemiluminescent first-overtone radiation at 2.7 μm from the reaction N+O₂ → NO+O, which is followed by the fast quenching reaction N+O → N₂+O. From the rate of overtone photons per O₂ molecule and the spectrum approximated by a Boltzmann distribution, they computed ?₂, the number of overtone photons per NO-forming reaction in the low-density limit when no quenching occurs. We show ?₂ is essentially independent of the spectrum, infer the limits on the fundamental-band photon efficiency, ?₁, and obtain the initial population distribution of NO(2 ? χ ? 6).     

O(1D)+N2O→NO+NO反应的理论研究

应用三体模型及扩展的LEPS势能面(PES),对初始条件为(Ecol=55 kJ/mol,v=0,j=0)的O(1D)+N2O→NO+NO反应体系进行了准经典轨线(QCT)计算.根据计算结果对体系的势能面及反应机理进行详细的分析和讨论,较全面地研究了此反应体系的动力学特征.     

The catalytic effects of H2CO3, CH3COOH,HCOOH and H2O on the addition reaction of CH2OO + H2O → CH2(OH)OOH

The addition reaction of CH₂OO + H₂O → CH₂(OH)OOH without and with X (X = H₂CO₃, CH₃COOH and HCOOH) and H₂O was studied at CCSD(T)/6-311+ G(3df,2dp)//B3LYP/6-311+G(2d,2p) level of theory. Our results show that X can catalyse CH₂OO + H₂O → CH₂(OH)OOH reaction both by increasing the number of rings, and by adding the size of the ring in which ring enlargement by COOH moiety of X inserting into CH₂OO···H₂O is favourable one. Water-assisted CH₂OO + H₂O → CH₂(OH)OOH can occur by H₂O moiety of (H₂O)₂ or the whole (H₂O)₂ forming cyclic structure with CH₂OO, where the latter form is more favourable. Because the concentration of H₂CO₃ is unknown, the influence of CH₃COOH, HCOOH and H₂O were calculated within 0–30 km altitude of the Earth's atmosphere. The results calculated within 0–5 km altitude show that H₂O and HCOOH have obvious effect on enhancing the rate with the enhancement factors are, respectively, 62.47%–77.26% and 0.04%–1.76%. Within 5–30 km altitude, HCOOH has obvious effect on enhancing the title rate with the enhancement factor of 2.69%–98.28%. However, compared with the reaction of CH₂OO + HCOOH, the rate of CH₂OO···H₂O + HCOOH is much slower.     

The electronic structures of the core and valence ion states of metal oxides

SCF-Xα SW MO calculations on metal core ion hole states and X-ray emission (XES) and X-ray photoelectron (XPS) transition states of the non- transition metal oxidic clusters MgO₆^10?, AlO₄^5? and SiO₄^4? show relative valence orbital energies to be virtually unaffected by the creation of valence orbital or metal core orbital holes. Accordingly, valence orbital energies derived from XPS and XES are directly comparable and may be correlated to generate empirical MO diagrams. In addition, charge relaxation about the metal core hole is small and valence orbital compositions are little changed in the core hole state. On the other hand, for the transition metal oxidic clusters FeO₆^10?, CrO₆^9? and TiO₆^8? relative valence orbital energies are sharply changed by a metal core orbital or crystal field orbital hole, the energy lowering of an orbital increasing with its degree of metal character. Consequently O 2p nonbonding → M 3d-O 2p antibonding (crystal field) energies are reduced, while M 3d bonding → O 2p nonbonding and M 3d-O 2p antibonding → M 4s,p-O 2p antibonding (conduction band) energies increase. Charge relaxation about the core hole is virtually complete in the transition metal oxides and substantial changes are observed in the composition of those valence orbitals with appreciable M 3d character. This change in composition is greater for e _g than for t_2g orbitals and increases as the separation of the e_g crystal field (CF) orbitals and the O 2p nonbonding orbital set decreases. Based on the hole state MO diagrams the higher energy XPS satellite in TiO₂ (at about 13 eV) is assigned to a valence → conduction band transition. The UV PES satellites at 8.2 eV in Cr₂O₃ and 9.3 eV in FeO are tentatively assigned to similar transitions to conduction band orbitals, although the closeness in energy of the crystal field and O 2p nonbonding orbitals in the valence orbital hole state prevents a definite assignment on energy criteria alone. However the calculations do clearly show that charge transfer transitions of the e_g bonding → e_g crystal field orbital type would generally occur at lower energy than is consistent with observed satellite structure.A core electron hole has little effect upon relative orbital energies and is only slightly neutralized by valence electron redistribution for MgO and SiO₂. For the transition metal oxides a core hole lowers the relative energies of M3d containing orbitals by large amounts, reducing O → M charge transfer and increasing M 3d crystal field → conduction band energies. Large and sometimes overcomplete neutralization of the core hole is observed, increasing from CrO₆^9? to FeO₆^10? to TiO₆^8?. as the O → M charge transfer energy declines.High energy XPS satellites in TiO₂ may be assigned to O 2p nonbonding → conduction band transitions while lower energy UV PES satellites in FeO and Cr₂O₃ arise from crystal field or O 2p nonbonding → conduction band excitations. Our “shake-up” assignment for FeO₆^10?, CrO₆^9? and TiO₆^8? are less than definitive because no procedure has yet been developed to calculate “shake-up” intensities resulting from transitions of the type described. However the results do allow a critical evaluation of earlier qualitative predictions of core and valence hole effects. First, we find that the comparison of hole or valence state ionic systems with equilibrium distance systems of higher nuclear and/or cation charge (e.g. the comparison of the FeO₆^10? Fe 2p core hole state to Co₃O₄) is dangerous. For example, larger MO distances in the ion states substantially reduce crystal field splittings. Second, core and CF orbital holes sharply reduce O → M charge transfer energies, giving 2e_g → 3e_g energy separations which are generally too small to match observed satellite energies. Third, highest occupied CF-conduction band energies are only about 4–5 eV in the ground states, but increase to about 7–11 eV in the core and valence hole states of the transition metal oxides studied. The energetic arguments presented thus support the idea of CF and/or O 2p nonbonding → conduction band excitations as assignments for “shake-up” satellites, at least in oxides of metals near the beginning of the transition series.