HeLi^n^+(n=0, 1)簇合物的稳定性和垂直激发态光谱

本文用ab initio研究了簇合物HeLi^n^+(n=0, 1)的几何构型和成键性质。在MP2(FULL)/6-31G**, 水平优化所得LeLi^+的平衡键长为0.2062nm, 与实验值0.205nm十分吻合。比较了HeLi^+(X^1∑^+和a^3∑^+), HeLi(X^2∑^+和a^4II)以及HLi(X^1∑^+)的稳定性, 计算了HeLi^+基态的相关能, 势能曲线和垂直激发态光谱。计算采用了6-31G**, 6-311G**,6-311G(2df, 2pd), 6-311G(3df, 2pd)和6-311+G(3df, 2pd)基组; 采用的方法包括MP2(FULL), MP4, MCSCF, MRSDCI, CCD和ST4CCD。计算表明, 同价HeLi^n^+中激发态的离解能均远比基态的大, 其中HeLi^+(a^3∑^+)的离解能最高(60.49kj/mol),说明激发态是稳定束缚态。HeLi^+基态比等电子体HLi分子基态的稳定性小得多。HeLi^+由A^1∑^+到B^1II的垂直跃迁(3σ→1π)振子强度较大而垂直跃迁能较小。     

BF分子X1∑+,A1∏和B1∑+电子态的势能函数

使用SAC/SAC-CI和D95＋＋,6-311＋＋g,6-311＋＋g^＊＊及D95（d）基组,分别对BF分子的基态X^1∑^＋、第一简并激发态A^1∏和第二激发态B^1∑^＋的平衡结构和谐振频率进行优化计算.对所有计算结果进行比较,得出6-311＋＋g^＊＊基组为最优基组.运用6-311＋＋g^＊＊基组和SAC方法对基态X^1∑^＋,SAC-CI方法对激发态A^1∏和B^1∑^＋进行单点能扫描计算,并用正规方程组拟合Murrell-Sorbie函数,得到相应电子态的势能函数解析式,由得到的势能函数计算了与X^1∑^＋,A^1∏和B^1∑^＋态相对应的光谱常数,结果与实验数据较为一致.     

PuX2+(X=O,H,N,C)分子离子的势能函数与稳定性

用密度泛函B3LYP方法对PuX2+(X=O,H,N,C)分子离子进行了理论研究,结果表明:PuO2+,PuH2+,PuN2+和PuC2+分子离子能稳定存在,基态电子状态是X5∑-(PuO2+),X8∑-(PuH2+),X4∑+(PuN2+)和X9∑-(PuC2+),势能函数为Murrell-Sorbie势函数,并导出了相应的几何性质,力学性质和光谱数据.     

化合物Mo(CO)~n^+(n=1～6)构型和键离能的密度泛函研究

采用DFT/B3LYP方法研究了化合物Mo(CO)~n^+(n=1～6)的基态可能构型,对于各n值,基态可能构型(电子态)依次为：直线型(^6∑^+),直线型(^6∑~g^+),C~2~υ(^2A~2)或D~3~h(^6A~1),D~4~H(^4A~1~g),C~2~ν(^2B~2)或C~4~ν'(^2B~1),D~3~d(^2A~1~g)。计算结果表明,对于n≥3时,碎片离子的构型与体系自旋多重度关系敏感。进一步计算了Mo－CO键的逐级解离能,计算值与实验结果能较好吻合,并从Mo原子4d和5s轨道杂化角度来解释该键解离能随n值的非单调变化。     

化合物Mo(CO)~n^+(n=1～6)构型和键离能的密度泛函研究

采用DFT/B3LYP方法研究了化合物Mo(CO)~n^+(n=1～6)的基态可能构型,对于各n值,基态可能构型(电子态)依次为：直线型(^6∑^+),直线型(^6∑~g^+),C~2~υ(^2A~2)或D~3~h(^6A~1),D~4~H(^4A~1~g),C~2~ν(^2B~2)或C~4~ν'(^2B~1),D~3~d(^2A~1~g)。计算结果表明,对于n≥3时,碎片离子的构型与体系自旋多重度关系敏感。进一步计算了Mo－CO键的逐级解离能,计算值与实验结果能较好吻合,并从Mo原子4d和5s轨道杂化角度来解释该键解离能随n值的非单调变化。     

键函数法与Be2体系的稳定性1: Be2的基态

采用价电子全CI(FCI)方法对Be2的基态(X^1∑g^+)进行了研究, 仔细考察了键函数在弱键体系计算中的作用。对引入键函数的不同方式分别按Boys方法计算了基组重叠误差(BSSE)。键函数的运用使得Be2基态性质的计算结果大为改善。研究结果表明键函数方法在相互作用能小的体系的计算中十分可取。     

键函数法与Be2体系的稳定性1: Be2的基态

采用价电子全CI(FCI)方法对Be2的基态(X^1∑g^+)进行了研究, 仔细考察了键函数在弱键体系计算中的作用。对引入键函数的不同方式分别按Boys方法计算了基组重叠误差(BSSE)。键函数的运用使得Be2基态性质的计算结果大为改善。研究结果表明键函数方法在相互作用能小的体系的计算中十分可取。     

胺对锂电池电解液中小分子的稳定作用

用密度泛函理论(DFT)方法在PBE0/6-31+G(d, p)水平上对乙胺、乙二胺分别与电解液中的小分子H2O、HF分子间的相互作用进行理论计算, 并在PBE/TZP 水平上利用能量分解分析(EDA)方法对胺与HF、H2O 结合的II-1、II-2、III-1和III-2模型进行计算分析. 结果表明, 胺类物质都能与HF、H2O形成N…H—F(O)、F(O)…H—N或F(O)…H—C的稳定氢键. 但HF与胺类物质形成的氢键比H2O与胺形成的氢键强, 故胺类物质在电解液中优先稳定HF. 乙二胺与HF、H2O结合的稳定性比乙胺强. 乙胺、乙二胺与HF(H2O)形成的最稳定构型均由F(O)—H…N 和F(O)…H—C 氢键结合形成.     

传能反应O（^1D）＋CO2（1∑g^＋）→O（^3P）＋CO2（1∑g^＋）中间物机理的理论研究

利用ab initio量子化学方法研究了自旋禁阻的传能反应O(^1D) CO2(1∑g^ )→O(^3P) CO2(1∑g^ )的反应机制，通过中间化合物CO3的单、三重态的势能面交叉点的确认，证明了中间物传能机理的可行性，同时计算了交叉点处的自旋-轨道偶合和面间跃迁几率，进一步证明了中间化合物CO3的形成在传能过程中的重要作用。     

轴不对称支撑的手性N-O酰胺化合物催化亚胺硅氢化反应的过渡态研究

利用Hartree-Fock(HF)算法和密度泛函理论(DFT)探讨了新型轴手性氮氧酰胺类配体催化亚胺C=N双键不对称硅氢化反应的过渡态.研究发现,H在Si原子上,反应经过渡态TS-2,能垒较低,由此得到产物(-)-N-(1-phenylethyl)aniline的e.e.值与实验结果相吻合.同时,本文还尝试采用合理的简化模型计算反应过渡态,其结果与使用全部分子用于过渡态能量计算的结论一致.     

Influence of electronic correlation in monoelectronic density in p-space

The radial molecular monoelectronic density and their orbital contributions have been calculated in the momentum space. For these purposes, densities for the ground state of several atoms and molecules, using a cc-pVTZ basis set at HF level, as well as some post-HF and DFT methods are computed. The difference between the radial monoelectronic density computed with each method and that using the HF wave function is used as a tool to study the influence of the electronic correlation in the momentum space. Densities obtained with post HF calculations show a similar behavior around p = 1.0 and 2.0, that are different from the DFT results. Radial momentum densities (p-densities) are more influenced by the electronic correlation than the exchange part of the DFT methods. CISD p-density is more affected than DFT p-density when the intermolecular distance increases. An analysis of the powers of moments calculated with different methods has been carried out. Contribution to the Serafin Fraga Memorial Issue.     

三氟化氯和环氧丙烷反应的理论研究

应用密度泛函理论对三氟化氯和环氧丙烷反应产生C3H5O和C1F2自由基的机理进行了研究。在B3PW91/6-31+G(d,p)水平优化了12个不同反应通道上各驻点(反应物、中间体、过渡态和产物) 的几何构型,并计算了它们的振动频率和零点振动能。采用CCSD(T)/6-31+ G(d,p) // B3PW91/6-31+G(d,p)单点能计算方法求得各物种的能量,并作了零点能校正。计算结果表明,三氟化氯和环氧丙烷反应可经过不同的反应路径引发C3H5O自由基和C1F2自由基,其中,三氟化氯呈对称的F原子与环氧丙烷的C(1)上与CH3在同一侧的上的H原子结合的活化能最低,仅为16.81 kJ/mol。     

环己烯分子2b和3a轨道的电子动量谱学研究

The electron momentum profile for inner valence orbitals 2b and 3a of cyclohexene (C6H10) was firstly studied by the binary (e,2e) electron momentum spectroscopy (EMS), at the impact energy of 1200 eV plus binding energy using symmetric non-coplanar kinematics. The complete valence shell binding energy spectrum of C6H10 was also obtained. The experimental momentum profile of the summed orbitals was compared with Hartree Fock (HF) and density functional theory (DFT) methods with various basis sets. The experimental measurement was well described by the HF and DFT calculations except for the low-p region (p<0.25 a.u.). Experimental small “turn-up” effects of momentum profile in the low-p region could be due to the distorted wave effects.     

Analysis of Vibration Mode for H_2+F→HF+H Reaction Mechanism: Density functional Theory Calculation

As one of the simplest chemical reactions A+BC→AB+C, the prototypical reaction, F+H2→HF+H , along with its isotopic variants, has been one of the most thoroughly investigated reactions in chemical reaction dynamics both in experimental and theoretical fields. For the A+BC?AB+C reaction, in the process of the A atom of initial state incoming towards the reaction region, provided that the interaction between A and BC is strong, according to the Franck-Condon principle, the internuclear…     

Synthesis and Electronic Properties of 6-Chloro-2-diethylaminoethyl-3(2H)-pyridazinone

6-Chloro-2-diethylaminoethyl-3(2H)-pyridazinone was synthesized by the reaction of 6-chloro-3(2H)-pyridazinone and 2-diethylamionethyl chloride reaction in methylbenzene.Then the structure was characterized by means of ^1H NMR,IR,UV.By the method of ab initio HF and density functional theory(DFT) BeLYP,the geometric structures of the reagent intermediate,the product and its isomer were optimized and their total energies were calculated,The properties for the frontier molecular orbitals and the rules for energy distribution were analyzed systematically.It was shown that the energy of the nitrogen alkyl compound is lower than that of the oxy alkyl compound and the former is stable than the latter.This result is in accordance with the fact that 6-chloro-2-diethylaminoethyl-3(2H)-pyridazinone is synthesized by the reaction of 6-chloride-2-diethylaminoethyl-3(2H)-pyridazinone and 2-diethylaminoethyl chloride.     

A theoretical study on N-phenyl-N'-(2-thienylmethylene)hydrazine

The molecular geometry and vibrational frequencies of N-phenyl-N'-(2-thienylmethylene)hydrazine (C11H10N2S) have been calculated using Hartree-Fock and density functional method (B3LYP) with 6-31G(d) basis set. The optimized geometric bond lengths and angles obtained using HF and DFT (B3LYP) are in agreement with the experimental data. B3LYP method seems to be appropriate than HF method for the calculation of vibrational frequencies and geometrical parameters of the (C11H10N2S) compound.     

Fully relativistic coupled cluster and DFT study of electric field gradients at Hg in 199Hg compounds

We investigate the magnitude and interplay of relativistic and electron correlation effects on the electric field gradient (EFG) at the position of Hg in linear and bent HgL(2) (L = CH(3), Cl, Br, I) and trigonal planar [HgCl(3)](-) compounds using four-component relativistic Dirac-Coulomb (DC) and non-relativistic (NR) calculations at the Hartree-Fock (HF), DFT, MP2 and coupled cluster (CC) levels. The relativistic and electron correlation contributions to EFG have opposite signs and are not additive, demonstrating the importance of taking into account relativistic and electron correlation contributions on an equal footing. DC-MP2 overestimates the electron correlation correction by 0.48-0.56 a.u. for Hg-halides and by 0.8 a.u. for Hg(CH(3))(2), respectively, while DC-CCSD underestimates the correlation correction by 0.57-0.66 a.u. compared to the reference DC-CCSD-T data. EFGs obtained at the DC-DFT level vary considerably with the functional; DC-CAMB3LYP and DC-BH&H reproduce DC-CCSD-T results within 0.08-0.24 a.u. (1%-3%) for Hg(CH(3))(2) and Hg-halides, respectively. An updated value of the nuclear quadrupole moment of the I = 5/2 excited state of (199)Hg, Q((199)Hg) = 0.675(12) b is derived from the literature. This value compares well with that derived from our calculated EFG at the DC-CCSD-T level and the experimental data for Hg(CH(3))(2); Q((199)Hg) = 0.650 b.