类卡宾H2C=CLiF的构型及其异构化

本文用解析梯度和RHF/STO-3G方法研究了锂卤类卡宾H2C=CLiF势能面的主要特征, 得到了四种平衡构型及其异构化的过渡态构型. 平衡构型的能量按三元环构型、四元环构型、σ-配合物构型和p-配合物构型的顺序递增. 文中分析了各构型的特点, 给出了偶极矩、电荷分布和前线分子轨道, 并对该类卡宾的化学反应性质进行了讨论.     

钠卤类硅烯的结构与稳定性

本文用RHF/STO-3G解析梯度方法研究了钠卤类硅烯H2SiNaX(X=F,Cl)势能面的主要特征, 得到了它们的几种平衡构型及其异构化的过渡态构型。与锂卤类硅烯相似, 三元环构型和P-配合物构型是最稳定的构型; 其它的两种构型-σ-配合物和经典"四面体", 也是势能面上的极值点, 但能量相对较高, 不稳定。文中对各构型的特点进行了分析。     

不饱和类硅烯H2C=SiNaCl的密度泛函理论研究

采用密度泛函理论方法,在B3LYP/6-311G(d,p)水平上研究了不饱和类硅烯H2C=SiNaCl的结构.结果表明,不饱和类硅烯H2C=SiNaCl共有4种平衡构型,其中非平面的p-配合物型构型能量最低,是不饱和类硅烯H2C=SiNaCl存在的主要构型.对平衡构型间异构化反应的过渡态进行了计算,求得了转化势垒.计算预言了最稳定构型的振动频率和红外强度.     

不饱和类卡宾H_2C=CLiF的密度泛函研究

采用量子化学中的密度泛函方法,在B3LYP/6-311G水平上全优化得到了不饱和类卡宾H2C=CLiF的平衡构型.结果表明,不饱和类卡宾H2C=CLiF只有2种平衡构型.对这2种平衡构型之间相互转化的过渡态进行计算,求得了转化势垒.根据计算得到的微观性质,采用统计热力学及过渡态理论,研究了2种平衡构型之间相互转化的热力学及动力学性质,进而讨论了2种平衡构型在不同温度下的稳定性问题.     

不饱和类硅烯H2C=SiNaF的DFT研究

用密度泛函理论方法, 在B3LYP/6-31+G(d, p)水平上研究了不饱和类硅烯H2C=SiNaF的结构. 结果表明, 不饱和类硅烯H2C=SiNaF共有四种平衡构型, 其中非平面的p-配合物型构型能量最低, 是不饱和类硅烯H2C=SiNaF存在的主要构型. 对平衡构型间异构化反应的过渡态进行了计算, 求得了转化势垒. 计算预言了最稳定构型的振动频率和红外强度.     

不饱和类卡宾H2C=CLiF的密度泛函研究

采用量子化学中的密度泛函方法,在B3LYP/6 311G水平上全优化得到了不饱和类卡宾H2C=CLiF的平衡构型.结果表明,不饱和类卡宾H2C=CLiF只有2种平衡构型.对这2种平衡构型之间相互转化的过渡态进行计算,求得了转化势垒.根据计算得到的微观性质,采用统计热力学及过渡态理论,研究了2种平衡构型之间相互转化的热力学及动力学性质,进而讨论了2种平衡构型在不同温度下的稳定性问题.     

不饱和类锗烯H2C=GeLiCl的DFT研究

采用密度泛函理论方法, 在B3LYP/6-311G(d, p)水平上研究了不饱和类锗烯H2C=GeLiCl的结构及异构化反应. 结果表明, 不饱和类锗烯H2C=GeLiCl有三种平衡构型, 其中非平面的p-配合物型构型能量最低, 是其存在的主要构型. 对平衡构型间异构化反应的过渡态进行了计算,求得了转化势垒. 计算预言了最稳定构型的振动频率和红外吸收强度.     

不饱和类锗烯H2C=GeNaBr的密度泛函理论研究

应用密度泛函理论DFT方法,在B3LYP/6-311G(d,p)水平上研究了不饱和类锗烯H2C=GeNaBr的结构及异构化反应.结果表明,不饱和类锗烯H2C=GeNaBr有3种平衡构型,其中非平面的p-配合物型构型能量最低,是其存在的主要构型.并对平衡构型间异构化反应的过渡态进行了计算,求得了转化势垒,预言了最稳定构型的振动频率和红外强度.     

不饱和类硅烯H_2CSiNaCl的密度泛函理论研究

采用密度泛函理论方法,在B3LYP/6-311G(d,p)水平上研究了不饱和类硅烯H2CSiNaCl的结构.结果表明,不饱和类硅烯H2CSiNaCl共有4种平衡构型,其中非平面的p-配合物型构型能量最低,是不饱和类硅烯H2CSiNaCl存在的主要构型.对平衡构型间异构化反应的过渡态进行了计算,求得了转化势垒.计算预言了最稳定构型的振动频率和红外强度.     

不饱和类锗烯H_2CGeNaBr的密度泛函理论研究

应用密度泛函理论DFT方法,在B3LYP/6-311G(d,p)水平上研究了不饱和类锗烯H2CGeNaBr的结构及异构化反应.结果表明,不饱和类锗烯H2CGeNaBr有3种平衡构型,其中非平面的p-配合物型构型能量最低,是其存在的主要构型.并对平衡构型间异构化反应的过渡态进行了计算,求得了转化势垒,预言了最稳定构型的振动频率和红外强度.     

类氮烯HNLiF构型和异构化反应理论研究

本文在量子化学从头算水平上, 用RHF/3-21G方法和梯度解析技术研究了类氮烯HNLiF势能面的主要特征, 得到三种平衡几何构型和两个异构化反应过渡态构型。平衡构型的能量按三元环构型、σ构型和p构型的顺序递增。三元环构型为类氮烯的主要存在形式。文中分析了各构型特点并给出其电荷分布和前线轨道。为用类氮烯合成含氮化合物提供了理论依据。     

Ion-pair dissociation dynamics of H2S in the photon energy range 15.26-15.55 eV

The H(+) velocity map images from the ion-pair dissociation of H(2)S + hν → SH(-)(X(1)Σ(+), υ = 0, 1) + H(+) have been measured at the excitation energies 15.259, 15.395, and 15.547 eV, respectively. The experimental results show that most of the available energies are transformed into the translational energies. The angular distributions of the fragments SH(-)(X(1)Σ(+), υ = 0) indicate that the dissociation occurs via pure parallel transition with limiting anisotropy parameter of +2. Because the ion-pair dissociation usually occurs via the predissociation of Rydberg states, this suggests that the ion cores of the excited Rydberg states have linear geometries. The geometries and electronic structures of the linear H(2)S(+) have been calculated employing the quantum chemistry calculation method at the CASPT2/avqz level. The electronic structures for the ion-pair states have been calculated at the CASSCF/avtz level, which indicates that the equilibrium geometries of the ion-pair states have bent geometries.     

A Theoretical Study on the Isomerization of HSOF System

1 INTRODUCTION The chemistry of atmospheric sulfur has beenlong studied due to its significant role in environmen-tal problems, such as acid rain, ozone and chemicalair pollution. To solve such problems, further know-ledge of the underlying processes involved in the at-mospheric sulfur cycle is necessary[1]. Moreover, de-tection of many sulfur-containing inorganic mole-cules in interstellar clouds has been reported. Thereactions of SO , an abundant ubiquitous interstellarion, with man…     

Structures and Electronic Properties of HOCl···HCOCl Complexes

B3LYP/6-311++G** and MP2/6-311++G** calculations were used to analyze the interaction between hypochlorous acid (HOCl) and formyl chloride (HCOCl). The results showed that there were four equilibrium geometries (S1, S2, S3, and S4) optimized at B3LYP/6-311++G** level, and all the equilibrium geometries were confirmed to be in stable states by analytical frequency calculations. Complexes S1 and S3 use the 5H atom of HOCl as proton donor and the terminal 1O atom of HCOCl as acceptor to form red shift hydrogen bond systems. However, the blue-shifted hydrogen bond (2C-3H···6O) coexists with 4Cl···5O interaction in structures S2. As for S4, it uses the 7Cl atom of HOCl as proton donor and the terminal 1O atom of HCOCl as acceptor to form red shift halogen bond system. Interaction energies between monomers in the four complexes corrected with basis set superposition error (BSSE) and zero-point vibrational energy (ZPVE) lie in the range from −5.05 to −14.76 kJ·mol⁻¹ at MP2/6-311++G** level. The natural bond orbital (NBO) and atoms in molecules (AIM) theories have also been applied to explain the structures and the properties of the complexes.     

Theoretical investigation of molecular properties of the first excited state of the thiophenoxyl radical

Accurate ab initio study of the lowest excited state (A (2)B(2)) of the thiophenoxyl radical is presented. The calculated equilibrium geometries, excitation energies, and harmonic vibrational frequencies show that the A (2)B(2) <-- X (2)B(1) excitation in C(6)H(5)S has different characteristics than the analogous transition in the phenoxyl radical. Vertical excitation energies for other low-lying (<4.5 eV) excited states of the thiophenoxyl radical are also presented and compared with available experimental data.     

A Theoretical Study on the Equilibrium Structures and Relative Stabilities of H_2SO

1INTRODUCTIONTheconformationandvariousphysicalprope-rtiesofdichalcogencompoundsR-X-Y-R?(X,Y=O,S,Se,andTe)havebeenatopicofseveralexperi-mentalandtheoreticalinvestigations[1].CompoundscontainingS=SandS=Obondshavelongbeenpro-posedasintermediatesinorganicsynthesisand,onoccasion,asstableentities[2～18].Despitethecom-monlyusedrepresentationofS–Obondinsulfoxi-desandothersulfinylderivativesasS=O,sulfoxidesareinmanywaysbestdescribedasylideswithhighlypolarizedS–Oσ-bondbecauseofelectro-sta…     

Theoretical characterization of the SiC3H- anion

Highly correlated ab initio methods are used to predict the equilibrium structures and spectroscopic parameters of the SiC(3)H(-) anion. The total energies and physical properties are reported using CASSCF/MRCI, RCCSD(T), and RCCSD(T)-F12 approaches and extended basis sets. The search of stable geometries leads to a total of 12 isomers (4 linear and 8 cyclic), for which electronic ground states have close-shell configurations. The stability of the linear form, l-SiC(3)H(-), is prominent. For the most stable linear isomer, the B(e) equilibrium rotational constant has been calculated with RCCSD(T) and a complete basis set. Core-correlation and vibrational effects have been taken into account to predict a B(0) of 2621.68 MHz for l-SiC(3)H(-) and 2460.48 MHz for l-SiC(3)D(-). The dipole moment of l-SiC(3)H(-) was found to be 2.9707 D with CASSCF/aug-cc-pV5Z and the electron affinity to be 2.7 eV with RCCSD(T)-F12A/aug-cc-pVTZ. Anharmonic spectroscopic parameters are derived from a quadratic, cubic, and quartic RCCSD(T)-F12A force field and second order perturbation theory. CASSCF/MRCI vertical excitations supply three metastable electronic states, (1)Σ(+) (3)Σ(+) and (3)Δ. Electron affinities calculated for a series of chains type SiC(n)H and SiC(n) (n=1-5) allow us to discuss the anion formation probabilities.     

HOCl…HCOCl复合物的结构和电子性质

在DFT-B3LYP/6-311++G**水平上求得HOCl+HCOCl复合物势能面上的四种稳定构型(S1,S2,S3和S4).其中,在复合物S1和S3中,HOCl单体的5H原子作为质子供体,与HCOCl单体中作为质子受体的10原子相互作用,形成红移氢键复合物;在复合物S4中,HOCl单体的7Cl原子作为质子供体,与HCOCl单体中作为质子受体的IO原子相互作用,形成红移卤键复合物;而在复合物S2中,同时存在2C-3H…6O蓝移氢键和4Cl…5O相互作用.在MP2/6-311++G**水平上计算的单体间的相互作用能考虑了基组重叠误差(BSSE)和零点振动能(ZPVE)校正,其值在-5.05与-14.76 kJ·mol-1之间.采用自然键轨道理论(NBO)对两种单体间相互作用的本质进行了考查,并通过分子中原子理论(AIM)分析了复合物中氢键和卤键键鞍点处的电子密度拓扑性质.     

Lowest electronic states of neutral and ionic LiN

We have investigated the potential energy curves (PECs) of the LiN heteronuclear diatomic molecule, including its ionic species LiN⁺ and LiN⁻, using explicitly correlated multi-reference configuration interaction (MRCI-F12) calculations in conjunction with the correlation consistent quintuple-𝜁 basis set. The effect of core–valence correlation, scalar relativistic effects, and the size of the basis sets has been investigated. A comprehensive set of spectroscopic constants determined based on the above-mentioned calculations are also reported for the lowest electronic states and all systems, including dissociation energies, harmonic and anharmonic vibrational frequencies, and rotational constants. Additional parameters, such as the dipole moments, equilibrium spin-orbit constants, excitation energies, and rovibrational energy levels, are also documented. We found that the three triplet states of LiN, namely, X ³∑⁻, A ³Π, and 2 ³∑⁻, exhibit substantial potential wells in the PEC diagrams, while the quintet states are repulsive in nature. The ground state of the anion also shows a deep potential well in the vicinity of its equilibrium geometry. In contrast, the ground and excited states of the cation are very loosely bound. Charge transfer properties of each of these states are also analyzed to obtain an in-depth understanding of the interatomic interactions. We found that the core–valence correlation has a substantial effect on the calculated spectroscopic constants.