采用量子波包方法和准经典轨线方法研究S(~3P)+HD反应

利用量子波包方法和准经典轨线方法在一个新的3A′′势能面上研究了S(3P)+HD→SD+H和SH+D反应的动力学性质.计算得到了两个反应通道在碰撞能为0.8—2.2 eV范围内的J=0反应几率、积分反应截面、内同位素因子和产物转动取向因子.这些结果揭示了S(3P)+HD反应非常明显的内同位素效应.通过对势能面和反应轨线的分析,我们发现了SD+H反应通道一个新的反应机制.S(3P)+HD反应的内同位素效应可以利用新发现的反应机制和反应的质量组合来进行解释.     

H/D/T+LiH反应的立体动力学研究

利用准经典轨线方法,在Prudente等人发表的LiH2体系势能面[Chem.Phys.Lett.474,18(2009)]上研究了原子分子反应H/D/T+ LiH→HH/HD/HT+ Li的立体动力学性质.在不同碰撞能下分别计算了该反应的反应截面,以及碰撞能为0.25 eV时的微分反应截面、角分布P(θr)、P(φr)和P(θr,φr).计算结果表明,随着碰撞能和攻击原子质量的增加,反应截面逐渐减小.对于所选定的碰撞能,当攻击原子质量增加时,反应产物向前散射趋势增强,向后散射的趋势几乎保持不变,产物的转动角动量j '取向程度增强并且定向于y轴负方向.     

H/D/T+LiH反应的立体动力学研究

利用准经典轨线方法,在Prudente 等人发表的LiH2体系势能面[Chem. Phys. Lett. 474, 18 (2009)]上研究了原子分子反应H/D/T+LiH →HH/HD/HT+Li的立体动力学性质。在不同碰撞能下分别计算了该反应的反应截面,以及碰撞能为0.25eV时的微分反应截面、角分布P(θr)。计算结果表明,随着碰撞能和攻击原子质量的增加,反应截面逐渐减小。对于所选定的碰撞能,当攻击原子质量增加时,反应产物向前散射趋势增强,向后散射的趋势几乎保持不变,产物的转动角动量j′取向程度增强并且定向于y轴负方向。     

F+HD→DF+H在中等碰撞能量下的反应立体动力学研究

采用准经典轨线（QCT）方法计算了F+HD→DF+H反应体系的立体动力学. 基于由 Alexander等人开发的势能面 (J. Chem. Phys. 113 (2000) 11084), 计算了该体系在碰撞能3.987Kcal/mol时的反应矢量相关性质,计算了极化微分反应截面（PDDCSs）随产物各振动量子数变量的变化.此外我们还计算了极角、方位角,讨论了产物的矢量性质. 计算结果验证了产物DF的前向散射性质,表明反应物转动量子数对该反应的矢量性有影响,同时本文也讨论了产物转动量子数 j''的定向问题.     

碰撞能对S(1D) +H2(v=0, j=0)→SH+H反应立体动力学性质的影响

利用1A′态的势能面[ Ho et al., J. Chem. Phys. 116, 4124 (2002)],采用准经典轨线方法研究了在不同碰撞能条件下,S(1D) +H2(v=0, j=0)→SH+H反应的立体动力学性质. 通过计算得到了描述反应物速度矢量k与产物的转动角动量矢量j′这两个矢量相关的分布函数P(r)、描述反应物速度矢量k、产物速度矢量k′与产物的转动角动量矢量j′这三个矢量相关的二面角分布函数P(r)以及描述反应产物角动量极化的分布函数P(r,r).计算结果表明产物的转动角动量矢量j′在空间具有明显的定向和取向效应,并且产物的转动角动量具有强烈的极化. 另外,计算结果还表明这些立体动力学性质对碰撞能非常敏感.     

碰撞能对S(1D) +H2(v=0, j=0)→SH+H反应立体动力学性质的影响

利用1A′态的势能面[ Ho et al., J. Chem. Phys. 116, 4124 (2002)]，采用准经典轨线方法研究了在不同碰撞能条件下，S(1D) +H2(v=0, j=0)→SH+H反应的立体动力学性质. 通过计算得到了描述反应物速度矢量k与产物的转动角动量矢量j′这两个矢量相关的分布函数P(r)、描述反应物速度矢量k、产物速度矢量k′与产物的转动角动量矢量j′这三个矢量相关的二面角分布函数P(r)以及描述反应产物角动量极化的分布函数P(r,r).计算结果表明产物的转动角动量矢量j′在空间具有明显的定向和取向效应，并且产物的转动角动量具有强烈的极化. 另外，计算结果还表明这些立体动力学性质对碰撞能非常敏感.     

碰撞能和同位素取代对H+BrF→HBr+F反应立体动力学影响的理论研究

基于拟合得到的London-Eyring-Polanyi-Sato势能面,运用准经典轨线方法对H+BrF→HBr+F反应的立体动力学性质进行了理论研究.计算了反映矢量相关的角分布和对光诱导的双分子反应实验敏感的四个极化微分散射截面.结果表明:随着碰撞能的增加,产物的转动极化变强,并且产物的后向散射占主导地位.通过比较D+BrF→DBr+F和H+BrF→HBr+F反应的产物极化,揭示了明显的同位素效应.     

Quasi-classical Trajectory Study of the Intramolecular Isotope Effect in the Reaction O(3P)+H2/HD

利用准经典轨线方法在BMS1解析势能面上研究了反应O(³P)+H₂体系的动力学性质. 主要研究了同位素效应对该反应体系的积分截面、产物转动态分布、微分截面、产物角动量的取向和定向以及对极化微分截面的影响. 对于微分截面,还考虑了反应物初始振动量子数对微分截面的影响. 对反应O+HD与O+H₂产生OH的转动发布进行比较,发现前者OH的转动激发更为明显. 微分截面的结果表明,振动量子数和同位素对散射方向有一定影响. 同位素取代对产物的取向和定向以及极化微分截面的影响也比较明显. 对以上结果利用已有的理论模型进行了分析,得到了合理的解释.     

O+DCl→OD+Cl反应的动力学性质研究

利用准经典轨线方法计算了O+DCl→OD+Cl反应的动力学性质.所得到的积分反应截面反映出该反应为典型的放热反应,这与势能面反应路径上没有能垒的特点一致.其微分反应截面的分布表明反应产物的前向散射和后向散射是不对称的,前向散射强于后向散射,因此该反应遵循间接反应机理,此机理通过对反应轨线进行抽样分析得到验证.反映两矢量K-J′相关的分布函数P(θr)和取向系数?P2(J′·K)?值的变化趋势均反映出产物分子OD的取向程度随碰撞能的增加先减弱后增强.反映三矢量K-K′-J′相关的二面角分布函数P(?r)表明产物分子转动角动量具有沿y轴的取向效应,当碰撞能较高时出现了比较明显的沿y轴正向的定向效应.随着碰撞能的增加,产物分子的转动由"平面内"机理向"平面外"机理过渡.     

O~+ + H_2及其同位素取代反应的立体动力学研究

运用准经典轨线方法,基于RODRIGO势能面,对碰撞能为20kcal/mol时,O++H2及其同位素取代反应的立体动力学性质进行了理论研究,对k-j′两矢量相关和k-k′-j′三矢量相关的分布函数、极化微分反应截面,以及产物转动取向参数进行了详细的讨论.结果表明,O++H2→OH++H,O++DH→OD++H和O++TH→OT++H反应的立体动力学性质对体系的质量因数非常敏感.     

反应物振动激发对O(3P)+D2→OD+D立体动力学的影响

运用准经典轨线方法,基于Roger的³A"势能面,在碰撞能为104.5 kJ/mol时对O(³P)+D₂反应的立体动力学性质进行了理论研究. 详细讨论与产物矢量相关的的极化分布函数以及四个极化微分反应截面进行了. 结果表明,产物OD的立体动力学性质对反应物分子H_{2相似文献}   

O+DC1→OD+Cl反应在~3 A″势能面上的动力学研究(英文)

在~3A″势能面上,在散射能为14～20 kcal/mol的范围内,运用准经典轨线方法对O+DCl→OD+Cl进行了动力学研究.我们发现积分散射截面随着散射能的增加而增大,产物OD的振动分布发生了很强的粒子数的反转现象,且振动激发较弱、转动激发较强.后向散射居于主导地位,碰撞能的变化对产物转动取向的影响不大.     

Quasi-classical trajectory approach to the O（1D）＋HBr ）OH＋Br reaction stereo-dynamics on X1A＇ potential energy surface

The vector properties of reaction O(¹D)+HBr→ OH+Br on the potential energy surface (PES) of X¹A′ ground singlet state are studied by using the quasi-classical trajectory (QCT) theory. The polarization-dependent differential cross sections (PDDCSs), the average rotational alignment factor 2(j′· k)>, as well as the distributions reflecting vector correlations are also computed. The analysis of the results shows that the alignment and the orientation distribution of the rotation angular momentum vector of product molecule OH is influenced by both the effect of heavy-light-heavy (HLH) type mass combination and the deep well of PES.     

Effects of reagent's rotational and vibrational excitations on reaction O(3P) + H2 H2(ν = 0, 3, j = 0, 3; 5; 7; 9; 12; 15) → OH + H

To investigate the effect of reagent's rotational and vibrational excitations on the stereo-dynamics of reaction product, the title reaction is theoretically simulated using the quasi-classical trajectory (QCT) method on the ³A" and ³A′ potential energy surfaces (PESs). The reaction cross section is considered as the only scalar property in this work at four different collision energies. Furthermore the vector properties including two polarization-dependent differential cross sections (PDDCSs), the angular distributions of product' rotational momentum are discussed at one fixed collision energy. Effects of reagents' rotational excitation on the reaction do exist regularly.     

Isotope effect on the stereodynamics for the collision reaction H＋LiF（v = 0, j = 0） → HF＋Li

Stereodynamics for the reaction H+LiF(v=0, j=0) → HF+Li and its isotopic variants on the ground-state (1 2 A′) potential energy surface (PES) are studied by employing the quasi-classical trajectory (QCT) method. At a collision energy of 1.0 eV, product rotational angular momentum distributions P (θr), P (φr), and P (θr ,φr), are calculated in the center-of-mass (CM) frame. The results demonstrate that the product rotational angular momentum j′ is not only aligned along the direction perpendicular to the reagent relative velocity vector k, but also oriented along the negative y axis. The four generalized polarization-dependent differential cross sections (PDDCSs) are also computed. The PDDCS 00 distribution shows a preferential forward scattering for the product angular distribution in each of the three isotopic reactions, which indicates that the title collision reaction is a direct reaction mechanism. The isotope effect on the stereodynamics is revealed and discussed in detail.     

Effect of reagent vibrational excitation and isotope substitution on the stereo-dynamics of the Ba+HF→BaF+H reaction

Based on an extended London-Eyring-Polanyi-Sato (LEPS) potential energy surface (PES), the Ba + HF reaction has been studied by the quasi-classical trajectory (QCT) method. The reaction integral cross section as a function of collision energy for the Ba + HF → BaF + H reaction is presented and the influence of isotope substitution on the differential cross sections (DCSs) and alignments of the product's rotational angular momentum have also been studied. The results suggest that the integral cross sections increase with increasing collision energy, and the vibrational excitation of the reagent has great influence on the DCS. In addition, the product's rotational polarization is very strong as a result of heavy-heavy-light (HHL) mass combination, and the distinct effect of isotope substitution on the stereodynamics is also revealed.     

Effects of a reagent＇s rotational and vibrational excitations on reactionO（3p）＋ H2（v=0, 3, j = 0, 3, 5, 7, 9, 12, 15） → OH ＋ H

To investigate the effect of a reagent’s rotational and vibrational excitations on the stereo-dynamics of the reaction product, the title reaction is theoretically simulated using the quasi-classical trajectory (QCT) method on the 3 A and 3 A potential energy surfaces (PESs). The reaction cross section is considered as the only scalar property in this work at four different collision energies. Furthermore the vector properties including two polarization-dependent differential cross sections (PDDCSs), the angular distributions of product’ rotational momentum are discussed at one fixed collision energy. Effects of reagents’ rotational excitation on the reaction do exist regularly.     

Product polarization distribution: Stereodynamics of the reaction of atom H and radical NH

The product angular momentum polarization of the reaction of H+NH is calculated via the quasiclassical trajectory method (QCT) based on the extended London-Eyring-Polanyi-Sato (LEPS) potential energy surface (PES) at a collision energy of 5.1 kcal/mol. The calculated results of the vector correlations are denoted by using the angular distribution functions. The polarization-dependent differential cross sections (PDDCSs) demonstrate that the rotational angular momentum of the product H₂ is aligned and oriented along the direction perpendicular to the scattering plane. Vector correlation shows that the angular momentum of the product H₂ is aligned in the plane perpendicular to the velocity vector. It suggests that the reaction proceeds preferentially when the reactant velocity vector lies in a plane containing all three atoms. The orientation and alignment of the product angular momentum affects the scattering direction of the product molecules. The polarization-dependent differential cross sections (PDD-CSs) reveal that scattering is predominantly in the backward hemisphere.     

The stereodynamic properties of the F+HO(v,j) → HF+O reaction on~1 A' and ~3A' potential energy surfaces by quasi-classical trajectory calculations:Initial excitation effect(v=1-3, j=0 and v= 0, j=1-3)

The stereodynamic properties of the F ＋ HO （v, j） reaction are explored by quasi-classical trajectory （QCT） calculations performed on the 1At and 3At potential energy surfaces （PESs）. Based on the polarization-dependent differential cross sections （PDDCSs） and the angular distributions of the product angular momentum with the reactant at different values of initial v or j, the results show that the product scattering and product polarization have strong links with initial vibrationalrotational numbers of v and j. The significant manifestation of the normal DCSs is that the forward scattering gradually becomes predominant with the initial vibrational excitation increasing, and the scattering angle of the HF product taking place on the 3At potential energy surface is found to be more sensitive to the initial value of v. The product orientation and alignment are strongly dependent on the initial rovibrational excitation effect. With enhancement in the initial rovibrational excitation effect, there is an overall decrease in the product orientation as well as in the product alignment either perpendicular to the reagent relative velocity vector k or along the direction of the y axis, for which the initial rotational excitation effect is much more noticeable than the vibrational excitation effect. Moreover, the initial rovibrational excitation effect on the product polarization is more pronounced for the 3At potential energy surface than for the 1At potential energy surface.