几种含芯电子相关能修正的G2和G2(ACI)方法

针对冻结芯电子近似,在MP2/6-311G(d,p)级别上对G2、MP2/6-311G(d)和MP2/6-311G(d,p)级别上对G2(QCI)方法进一步考虑了芯电子相关能修正,尝试建立了G2(fu2)、G2(QCI/ful)和G2(QCI/fu2)方法。G2-l test set 的反应能量计算结果表明,这些方法进一步减小了经验修正量;G2(QCI/ful)和G2(QCI/fu2)也比G2(QCI)的总体精度有所提高;但G2(fu2)在G2基础上,总体精度没有改善。G2(fu2)、G2(QCI/ful)和G2(QCI/fu2)计算G2-l test set反应能量的平均绝对偏差分别为5.11、4.74和4.81kJ mol-1,G2和G2(QCI)分别为5.09和4.97kJ mol-1.     

含芯电子相关能修正的G2理论——G2(ful)

A general method in considering the core electronic correlation energies has been proposed and introduced into the standard Gaussian-2 (G2)[7] theory by small post-Hartree-Fock calculations. In this paper an additional MP2(FC)/6-31G(d) calculation over the G2 procedures is employed and examined in modification in modification to the flaw of Frozen-Core (FC) approximation of G2 vai eq.:
ΔE(full)= E[MP2(full)/6-31G(d)]-E[MP2(FC)/6-31G(d)]
where the MP2(full)/6-31G(d) energy has been obtained in the molecular geometry optimizations. This energy, ΔE(full), is directly added into the total G2 energy of a molecule in facilitating the effect of core electronic correlations for each molecule in chemical reactions. It has been shown that the over-all average absolute deviation for the 125 reaction energies of the G2 test set (test set 1) is slightly reduced from 5.09 to 5.01 kJ, mol(-1) while for the 55 D0 values, which have been used for the derivation of the A coefficient of the empirical High-Level...更多-Correction (HLC), it is also reduced from 4.99 [for both G2 and G2(COMPLETE)[8]]to 4.77 kJ• mol(-1). In addition, larger errors (greater than ±8.4 kJ•mol(-1) for the D0 energies are improved, especially for the largest error of the D0 of SO2 This error is reduced from 21.3 to 15.4 kJ. mol(-1), in which the experimental geometry would further reduce it by 7.1kJ.mol(-1)[8]. Another improvement is the absolute value of the A coefficient in HLC being reduced from 4.81 for G2 to 4.34 milli-hartrees which is believed to be useful in isolating the relationship between the HLC and the FC approximation. Modifications to the original G2 from this work is denoted as G2(fu 1) and thus the G2 (fu 1) total energy for a molecule is
E[G2(fu 1)]= E[G2]+Δ E(full)h
with a new ΔE[HLC] =-0.19α- 4.34nβ milli-hartree.     

Criegee中间体气相反应热力学的G2理论计算

Criegee intermediate is believed to play an important role in the atmospheric chemistry. Because of its short life and the difficulty in experimental study, we carried out ah initio calculations on the thermochemistry of the Criegee involving reactions in this study. Thermochemistry data of reaction enthalpies and Gibbs free energies for four different stable structures of the Criegee intermediates (singlet CH2OO ①1 A1 in C2v, triplet CH2OO ②3B1 in C2v, singlet CH2OO ③1A' in Cs and triplet CH2OO ④ in C1 symmetry) involved in some of the gas-phase reactions were calculated at the standard Gaussian-2 [G2(MP2) and G2] and a modified G2, G2(fu1)[10],levels of theory. Relative energies among those Criegees and formic acid were compared. Chemical reactions include the formation of Criegees, re-arrangement from Criegee to formic acid, dissociations (producing CH2(3B1)+O2, CH2(1A1)+O2, CO2+H2, CO2+2H, CO+H2O, OH+HCO) and the reactions between Criegee and NO/H2O. Standard equilibrium constants for some reactions were investigated and may be obtained for all of the rest reactions involved in this study by the standard Gibbs free energies. It is shown that the formation of Criegee ①-④ by ethylene and ozone, the re-arrangement from any Criegee to formic acid, the dissociation in producing CO2+O2and CO+H2O and the reactions between any Criegee and NO/H2O are all favourable thermodynamicaly. The dissociation in forming CO2+2H and OH+HCO is less favourable. While the dissociation in forming carbene (either in 3B1 or 1A1 state) is not allowed by ΔrGm? values. Standard enthalpies of formation at 298 K for the four Criegees were predicted at the G2(ful) level of theory. Each value is the average value from ten of the above reactions and they are -4.3, 74.8,98.9 and 244.6 kJ mol-1 at the G2(ful) level for Criegee ① to Criegee ④, respectively. In addition, tile standard enthalpy of formation at 298 K for HOCH2OOH is further predicted to be -315.6 kJ mol-1 at the G2(MP2) level.     

CH2FCF3与O(1D)反应机理的理论研究

用量子化学密度泛函理论(DFT)和G3(MP2)B3方法,对O(1↑D)与CH2FCF3的反应进行了研究．在UB3LYP/6-31G(d)计算水平上,优化了反应势能面上各驻点的几何结构,在G3(MP2)B3水平上进行了单点计算,并利用UB3LYP/6-311 G(3df,3pd)计算的波函数进行了电荷密度分析．通过内禀坐标(IRC)计算和振动分析,对反应过渡态进行了确认,并确定了反应机理．     

CH2(～X3B1)与NO的基元化学反应研究

The reaction of methylene radicals in their 3B1 electronic ground state with molecular NO was studied. Pure CH2(～X3B1) radicals were produced by UV photolysis of ketene at 351 nm. The products were measured by Time-Resolved Fourier Transform Infrared (TR-FTIR) spectrometer. CO、OH、NH2 and HOCN or its isomer HNCO were found as primary products and several possible channels of this reaction were suggested.     

Eu(OPri)3/Tb(OPri)3共掺杂P(MMA-co-St)

Eu(OPri)3/Tb(OPri)3共掺杂P(MMA-co-St);Eu(OPri)3/Tb(OPri)3;共掺杂;P(MMA-co-St);荧光性能     

PbMg1/3Nb2/3O3 (PMN)和PbMg1/3Nb2/3-PbTiO3 (PMNT)中几种局域结构与晶格形变的从头算研究

建立了钙钛矿结构铌镁酸铅PbMg1/3Nb2/3O3(PMN)的2×2×3复晶胞模型; 采用ab initio方法讨论了PMN晶体各种可能构型的稳定性; 选取了PMN三种高、中、低稳定性的代表构型, 并对Ti替换B位离子后的结构进行了结构优化. 计算结果表明复晶胞刚性模型的最低和最高能量差约0.74 a.u. (1940 kJ); Pb2＋离子结构框架的形变是PMN晶格发生形变的主要因素; 在不考虑被替换离子电荷差异的情况下, MgO6含量越少越有利于Ti离子替换Nb与晶胞的形变. PMNT材料中构型的分布和局域形变取决于生长PMNT材料的工艺过程.     

Ru(bipy)_3~(2 )/Ru(phen)_3~(2 )-C_2O_4~(2-)-Ce~(IV)化学发光反应动力学模型的研究

根据Ru(bipy)_3~(2 )/Ru(phen)_3~(2 )-C_2O_4~(2-)-Ce~Ⅳ(bipy=2,2＇-联吡啶,phen=1,10-邻菲咯琳)化学发光反应建立了该化学发光反应的动力学模型,根据模型计算出该反应的发光强度-反应时间曲线上升及下降阶段的反应速率常数、发光强度最大值及其出现的时间等.发光强度最大值及发光强度-反应时间曲线下的面积均可用于定量分析.     

Ru(bipy)2+3/Ru(phen)2+3-C2O2-4-CeⅣ化学发光反应动力学模型的研究

根据Ru(bipy)2+3/Ru(phen)2+3-C2O2-4-CeⅣ(bipy=2,2′-联吡啶,phen=1,10-邻菲咯啉)化学发光反应建立了该化学发光反应的动力学模型,根据模型计算出该反应的发光强度-反应时间曲线上升及下降阶段的反应速率常数、发光强度最大值及其出现的时间等.发光强度最大值及发光强度-反应时间曲线下的面积均可用于定量分析.     

Dy_(2)O_(3),Cu_(2)O在LiF-DyF_(3)熔盐体系的溶解度研究EI北大核心CSCD

以LiF-DyF_(3)为熔盐,电解Dy_(2)O_(3),Cu_(2)O制备Dy-Cu合金过程中,明确Dy_(2)O_(3),Cu_(2)O溶解度是制定合理加料制度、提高电解效率的关键。采用等温饱和法研究了Dy_(2)O_(3),Cu_(2)O溶解平衡时间,考察了温度、DyF_(3)浓度对单一氧化物(Dy_(2)O_(3)或Cu_(2)O)及混合氧化物(Dy_(2)O_(3)与Cu_(2)O)溶解度的影响,通过最小二乘法对溶解度数据进行了拟合,建立了温度、DyF_(3)浓度与Dy_(2)O_(3),Cu_(2)O溶解度之间的数学回归方程。研究结果表明,Dy_(2)O_(3),Cu_(2)O在LiF-DyF_(3)熔盐中溶解平衡的时间分别为110,120 min,溶解反应为吸热反应。相同温度下,随熔盐中DyF_(3)浓度增大,Dy_(2)O_(3)的溶解度逐渐增大,Cu_(2)O溶解度变化较小;在温度为910~1030℃,熔盐中DyF_(3)浓度为15%~40%(摩尔分数)时,Dy_(2)O_(3),Cu_(2)O溶解度分别为0.55%~3.45%,0.39%~0.52%。     

亚烷基锡烯与乙烯环加成反应机理的理论研究

The mechanism of a cycloaddition reaction between singlet alkylidenestannylene and ethylene has been investigated with MP2/3-21 G^* and B3LYP/3-21 G* methods, including geometry optimization and vibrational analysis for the involved stationary points on the potential energy surface. Energies for the involved conformations were calculated by CCSD(T)//MP2/3-2 IG^* and CCSD(T)//B3LYP/3-21G^* methods, respectively. The results show that the dominant reaction pathway of the cycloaddition is that an intermediate (INT) is firstly formed between the two reactants through a barrier-free exothermic reaction of 39.7 kJ/mol, and the intermediate then isomerizes to a four-membered ring product (P2.1) via a transition state TS2.1 with a barrier of 66.8 kJ/mol.     

O（~1D）与CF_2HCl反应的理论研究

用量子化学密度泛函理论（DFT）和G3B3方法，对为（~1D）与CF_2HCl的反应 进行了研究，在B3LYP/6-311+G(d)，B3LYP/6-311+G(2df,2pd)和G3B3计算水平上， 优化了反应热能面上各驻点的几何结构，通过内禀反应坐标（IRC）计算和振动分 析，对反应过渡态进行了确认，并确定了反应机理。     

On the NH3+HCO3H→HCOOH+H3NO mechanism: a density functional theory study

The B1LYP, B3LYP and MPW1PW91 density functional theory methods combined with the 6-311G(2d, 2p) basis set were used to carry out a density functional theory study of the NH₃+HCO₃H→HCOOH+H₃NO reaction. The purpose of this work is to study the reaction mechanism from the viewpoint of bond order transformations throughout the course of the reaction, and propose the reasons for the apparent differences in activation barriers.     

PbMg1/3Nb2/3O3(PMN)和PbMg1/3Nb2/3-PbTiO3(PMNT)中几咱种局域结构与晶格形变的从头算研究

建立了钙钛矿结构铌镁酸铅PbMg1/3Nb2/3O3(PMN)的2×2×3复晶胞模型;采用ab initio方法讨论了PMN晶体各种可能构型的稳定性:选取了PMN 三种高、中、低稳定性的代表构型,并对Ti替换B位离子后的结构进行了结构优化.计算结果表明复晶胞刚性模犁的最低和最高能量差约0.74 a.u.(1940 kJ);Pb2+离子结构框架的形变是PMN晶格发生形变的丰要因素;在不考虑被替换离子电荷差异的情况下,MgO6含量越少越有利于Ti离子替换Nb与晶胞的形变.PMNT材料中构型的分布和局域形变取决于生长PMNT材料的工艺过程.     

NH2(～X2B1)与CH4反应机理的理论研究

在密度泛函理论B3LYP／6－311G^*水平下，研究了NH2与CH4的反应机理。通过振动频率和内禀反应坐标（IRC）分析，对反应过渡态进行了确认。在QCISD（T）／6－311G^*水平下进行了单点能计算，并进行了零点能校正，结果表明，反应NH2＋CH4→N3＋CH3是主要的反应通道。     

CH3SOCH3与XO(X=Cl,Br)自由基反应的理论研究

采用密度泛函理论B3LYP方法,在6-311 G(d,p)基组水平上研究了二甲亚砜(DMSO)与XO(X=Cl,Br)自由基反应的微观动力学机理,并利用经过wigner校正的传统过渡态理论计算了标题反应在200~2000 K温度范围内的反应速率常数。研究结果表明,DMSO与XO(X=Cl,Br)自由基反应主要有氧转移和抽氢两种反应机理,氧转移反应的能垒显著低于抽氢反应,且前者为放热反应后者为吸热反应;低温时氧转移反应占绝对优势,298 K时DMSO与XO(X=Cl,Br)两个反应体系的总速率常数分别为2.09×10-15和1.75×10-14cm3.molecu le-1.s-1,氧转移反应分支比均为100%。高温时抽氢反应上升为主通道。2000 K时其总速率常数分别为6.32×10-12和8.41×10-12cm3.molecule-1.s-1,抽氢反应分支比分别为91.8%和79.4%。