原子-多原子分子反应的含时波包理论研究

基于Modified Jordan和Gilbert的势能面,运用SVRT(semirigid vibrating rotor target)模型和TDWP(Time-Dependent Wave Packet)方法,对D+CH4,O(3P)+CH4反应体系进行了含时波包动力学研究,计算得到了不同初始振动态的总反应几率,总散射截面和热速率常数.通过对j=0时,v=0,1的反应几率的计算,看出H-CH3的振动激发,极大地提高了反应几率,而反应阈能明显降低,说明反应分子的振动能对分子的碰撞反应有重要贡献.     

D+CD4→CD3+D2反应的四维量子散射计算

运用约化维数量子动力学理论 ,利用含时波包法 ,对反应D +CD4 →CD3+D2 进行了四维量子散射计算 .将反应多原子CD4 看作双原子D—CD3,反应D +CD4 →CD3+D2 看作单原子 双原子反应 ,把体系的反应简化为四维散射问题 .波函数的传播采用分裂算符法 ,为避免格点边界处含时波函数的边界反射 ,采用了光学吸收势法 ,在格点边界处引入光学势 ,消除边界反射 .根据CD4 分子的C3v对称性 ,选取了Jordan和Gilbert提出的半经验势能面 .计算结果表明 ,反应概率随平动能的变化图像 ,呈现出显著的量子共振特性 ,这是很多提取反应的共同特征 .而不同振动态下的反应概率随平动能的变化表明 ,随振动量子数的增大 ,反应概率有明显提高 ,且反应阈能明显降低 ,这说明反应分子的振动能对分子的碰撞反应有重要贡献 .而对基态和第一振动激发态时散射截面的计算 ,也证明了这一结论 .同时 ,还分别通过计算量子数j,k ,m对反应概率的影响 ,对该反应的空间取向效应进行了研究 ,并与H +CH4→CH3+H2 反应进行了比较 .     

原子-多原子分子反应的含时波包理论研究

基于Modified Jordan和Gilbert的势能面，运用SVRT(semirigid vibrating rotor target)模型和TDWP(Time-Dependent Wave Packet)方法，对D CH4，O(^3P) CH4反应体系进行了含时波包动力学研究，计算得到了不同初始振动态的总反应几率，总散射截面和热速率常数。通过对j=0时，v=0，1的反应几率的计算，看出H—CH3的振动激发，极大地提高了反应几率，而反应阈能明显降低，说明反应分子的振动能对分子的碰撞反应有重要贡献。     

CH3与NO2的反应

用时间分辨傅立叶红外光谱法和量子化学计算，研究了CH3自由基与NO2的基元反应．由248 nm激光光解CH3Br或CH3I得到CH3自由基．首次观测到了振动激发的产物OH、HNO和CO2．另一产物NO也被证实．由此确定了反应通道CH3O+NO，CH2NO+OH 和HNO+H2CO．其中CH3O+NO是主要的反应通道．还用CCSD(T)/6-311++G(df,p)//MP2/6-311G(d,p)的方法对上述通道的机理在理论上做了研究．理论计算的结果与实验观察相符．     

CH3CH2O及CH3CHOH与HO2反应机理的理论研究

采用CCSD(T)/cc-pVTZ//B3LYP/6-311++G(2df,2p)水平上对CH3CHOH + HO2和CH3CH2O + HO2反应体系的单、三重态反应机理进行了详细的理论研究.计算结果表明,CH3CHOH + HO2反应主要发生在单重态势能面上,其中四条通道均为快速自发过程;CH3CH2O + HO2反应在三重态势能面上的通道CH3CH2O + HO2 → 3IM11 → 3TS11 → P11 (CH3CH2OH + 3O2)为动力学和热力学的优势路径. 大气中CH3CHOH比CH3CH2O更容易稳定存在.     

CH3CH2O及CH3CHOH与HO2反应机理的理论研究

采用CCSD(T)/cc-pVTZ//B3LYP/6-311++G(2df,2p)水平上对CH3CHOH + HO2和CH3CH2O + HO2反应体系的单、三重态反应机理进行了详细的理论研究.计算结果表明,CH3CHOH + HO2反应主要发生在单重态势能面上,其中四条通道均为快速自发过程;CH3CH2O + HO2反应在三重态势能面上的通道CH3CH2O + HO2 → 3IM11 → 3TS11 → P11 (CH3CH2OH + 3O2)为动力学和热力学的优势路径. 大气中CH3CHOH比CH3CH2O更容易稳定存在.     

SiH4+H→H2+SiH3反应的约化维数计算

对SiH4+ H→H2+SiH3反应体系应用SVRT模型进行了4维的量子动力学计算.将得到的速率常数与实验数据以及其他理论方法进行比较,得出了一些有意义的结论,并与CH4+H→H2+CH3反应在同种理论模型下做了对比,较好的与实验相吻合.最后验证了理论方法以及势能面的正确性.     

CH3CHF2与VO2+的反应机理

采用密度泛函方法在B3LYP/ 6-311G (2d, p)水平上研究了CH3CHF2与VO2+反应生成CH2=CF2 (H2消除反应), CH2=CHF(HF消除反应)和CH3CFO的机理。计算结果表明以上三种反应中,H2消除反应最容易发生。计算结果证明了相邻碳原子上的氢原子有利于C-F键的断裂。     

CH3CHF2与VO2+的反应机理

采用密度泛函方法在B3LYP/ 6-311G (2d, p)水平上研究了CH3CHF2与VO2+反应生成CH2=CF2 (H2消除反应), CH2=CHF(HF消除反应)和CH3CFO的机理。计算结果表明以上三种反应中,H2消除反应最容易发生。计算结果证明了相邻碳原子上的氢原子有利于C-F键的断裂。     

Cu~+、Ag~+、Au~+与乙硫醇的气相化学反应

利用激光溅射 分子束的技术 ,结合反射飞行时间质谱计 ,研究了Cu+、Ag+、Au+与乙硫醇的气相化学反应。结果显示这三种金属离子与 (CH3 CH2 SH) n 反应形成一系列团簇离子M+(CH3 CH2 SH) n,且团簇离子尺寸不一样。Ag+、Au+与乙硫醇的反应还生成了 (CH3 CH2 SH) +n ,由此推测Cu+、Ag+、Au+与乙硫醇团簇的反应存在两种通道 ,一种通道是生成M+(CH3 CH2 SH) n,另一种是生成 (CH3 CH2 SH) +n 。Cu+、Au+与乙硫醇的反应还生成了M+(H2 S) (M =Cu、Au) ,但是实验中没有观察到Ag+(H2 S) ,理论计算表明Ag+(H2 S)很不稳定。另外 ,分析产物离子M+(CH3 CH2 SH) n 的强度发现 ,n =1～ 2之间存在明显的强度突变现象     

Insights into the Maillard reaction. The mechanism of Schiff's base formation from the reaction force perspective

Schiff's base formation of the Maillard reaction is described from a theoretical viewpoint. The double proton transfer reaction was investigated within the frame of reaction force analysis in which global and local electronic properties were monitored within reaction regions defined along the reaction coordinate. Calculations based on density functional theory show that Schiff's base formation in the Maillard reaction occurs through an asynchronous double proton transfer, the second proton transfer being the determinant step of the reaction.     

Radiative lifetimes for the A2Σ+ (v′ = 0–7) and D2Σ+ (v′ = 0–5) Rydberg states of NO

Intensities for the γ(A²Σ⁺?→?X²Π), ε(D²Σ⁺?→?X²Π) and (D²Σ⁺?→?A²Σ⁺) bands for NO have been calculated using the Molecular Quantum Defect Orbital (MQDO) methodology. Radiative lifetimes for the A²Σ⁺ and D²Σ⁺ vibrational Rydberg states have also been determined. The present results are in excellent accord with measurements available in the literature. Additionally, predictions for a number of unknown intensities and radiative lifetimes are made, given their potential usefulness.     

CO2 production in the bromate‐1,4‐cyclohexanedione oscillatory reaction

NMR and GC/MS spectroscopy of the organic extracts of the oscillatory bromate‐1,4‐cyclohexanedione reaction illustrate the presence of ring‐opening products 5‐(dibromomethylene)‐2(5H)‐furanone, (E)‐5,5,5‐tribromo‐4‐oxo‐2‐pentenoic acid, and dibromoacetic acid, particularly at elevated temperatures. The loss of a carbon atom from the six‐membered ring after ring opening led to gas formation and such a process became more vigorous at >60 °C, with the direct observation of bubbles in a stirred batch reactor. Gravimetric experiments confirm that the amount of carbon dioxide gas produced increases rapidly with reaction temperature. Parallel experiments suggest that the ring‐opening process involves the oxidation of brominated benzoquinones by bromate. Copyright © 2010 John Wiley & Sons, Ltd.     

A statistical model for predicting thermal chemical reaction rate

A simple model based on the statistics of individual atoms [Europhys. Lett. 94 40002 （2011）] or molecules [Chin. Phys. Lett. 29 080504 （2012）] was used to predict chemical reaction rates without empirical parameters, and its physical basis was further investigated both theoretically and via MD simulations. The model was successfully applied to some reactions of extensive experimental data, showing that the model is significantly better than the conventional transition state theory. It is worth noting that the prediction of the model on ab initio level is much easier than the transition state theory or unimolecular RRKM theory.     

Study of the structure of unstable nuclei through the reaction experiments

Along with the development of the radioactive nuclear beam facility, the study of the structure of unstable nuclei has progressed rapidly over the last few decades. Due to the weakly binding property, the structure information of the unstable nuclei comes primarily from the scattering or reaction experiments. Therefore it would be very important to understand clearly the reaction mechanism involved in the experiment. We outlined here the major reaction mechanisms which are adequate to the study of unstable ...     

碳化硅合成反应动力学研究

基于经典轨迹法研究了碳化硅合成反应C(3Pg) SiO(X1∑ ,V=0,1;J=0)→SiC(X1∑ ) O(3Pg)的动力学.该反应存在阈能,反应截面均存在一个极大值和最佳反应能量.当SiO(X1∑ )分别处于V=0、J=0和V=1、J=0状态时,反应阈能分别约为1.2552×103kJ.mol-1和1.1297×103kJ.mol-1,反应截面极大值分别为5.3742×10-3nm2和5.1824×10-3nm2,而最佳初始碰撞能Et(the Optimal InitialCollision Translation Energy)分别为3.3472×103kJ.mol-1和3.7656×103kJ.mol-1.在SiC的最佳产率区(即最佳反应能区),通过反应物的振动激发并不能使SiC产率明显提高,因此基态下SiC合成反应的最佳能区即为该反应的最佳产率区.     

2H-氮杂卓衍生物迁移反应的光谱学特征

氮杂卓化合物存在1H-,2H-,3H-和4H-共4个互变异构体,其中,2H-,3H-系统是最重要的。2H-氮杂卓母体化合物很不稳定,4位存在叔-丁基,并且环上含有丙硫基(PrS-)取代基的2H-氮杂卓,不仅发生H迁移,也能发生PrS-迁移,向较稳定的3H-氮杂卓异构化。以2,7-二甲氧基-4-甲基-2H-氮杂卓为原料,通过与Pr-SH的取代反应,合成7-甲氧基-4-甲基-2-PrS-2H-氮杂卓,并讨论分析产物的 迁移反应。通过IR、¹H NMR、¹³C NMR、MS检测表明,在室温条件下,4位存在甲基的2H-氮杂卓衍生物,选择性地发生 PrS-迁移,生成3H-氮杂卓,而且此异构化反应速度比叔-丁基存在时的情况更快。     

The (n, α) reaction on 11B induced by 14.4 MeV neutrons

The ¹¹B(n, α)⁸Li reaction has been studied at 14.4 MeV in a geometry that allows simultaneous detection of the emitted and recoil particles. The angular distributions have been measured for the transitions to the ground and first excited states of the ⁸i nucleus and compared with PWBA for knock-on and heavy-particle pick-up processes. The total cross sections for the respective transitions have been deduced.     

Elastic pion-deuteron scattering near the 3-3 resonance

The elastic scattering of positive pions by deuterium has been studied at seven energies between 82 MeV and 292 MeV laboratory kinetic energy in the angular range between 30° and 130° (lab). The results are compared to recent relativistic three-body calculations.     

Quasi-free scattering of polarized protons

Cross section and analyzing power, energy-sharing spectra have been measured for the ¹⁶O($\text{p}$, 2p) reaction at an incident energy of 200 MeV for twenty-four different pairs of angles of the detected final-state protons. This general survey is intended to test the validity of the distorted wave impulse approximation (DWIA), particularly with respect to the predicted j-dependent analyzing power caused by the distorting optical potentials and nuclear spin-orbit coupling. Although the data in general confirm this j-dependence, agreement in detail between DWIA calculations and the analyzing power data becomes worse as the momentum of the recoiling nucleus increases. Predictably, the cross-section calculations show more sensitivity to the optical-model parameters than do the analyzing powers. Within the present limits imposed by scanty elastic scattering data, there seems to remain a choice between predicted ($\text{p}$, 2p) cross sections which either are unreasonably large or which have the incorrect energy-sharing shapes. More comprehensive elastic scattering and total reaction cross section data are clearly needed.