Jahn－Teller变形后C60－的结构和电子光谱

用INDO系列方法对C₆₀^－进行几何构型优化,得到D_3d对称性的构型,表明C₆₀^－确实发生了Jahn-Teller畸变,导致单键变短,双键变长,形成10种键,6种不等同碳原子,并以此构型为基础,计算了C₆₀^－的电子光谱,与实验结果吻合;同时对光谱进行了理论指认;最后对C₆₀^－的3种构型：D_5d,D_3d,D_2h的几何构型、能量、光谱和反应特性进行了分析、比较和总结。     

C40H2各种可能异构体稳定性的理论研究

采用AM1和PM3两种半经验方法,对D_5d对称性的C₄₀及C₄₀H₂所有可能异构体的几何构型进行了非限制对称性全优化,得到51种稳定异构体,在此基础上研究了氢的加成反应规律及本体C₄₀和最稳定及最不稳定C₄₀H₂异构体的红外光谱,讨论了影响C₄₀(D_5d)氢加成异构体稳定性及加成位置选择性的三种主要因素:(1)C₄₀本体几何结构;(2)共轭效应;(3)电荷分布影响.     

C36H2异构体的稳定性及其加成位置选择性的研究

使用AM1和PM3两种半经验方法,对所有的C₃₆H₂异构体实行非对称性限制的全优化,并结合频率分析及HF/6-31G单点能计算,确定了各异构体的基态结构及其相对稳定性.在此基础上,通过分析加成位置与异构体稳定性之间的关系,得出三条加成位置选择性的规律.最后,利用π-轨道轴矢量(POAV)方法计算了反应前后碳笼中张力的变化.张力与键级分析的结果表明加成位置选择性的规律不是由碳笼释放的张力决定的,而是由C₃₆H₂体系的总共轭性质决定的.     

NiTi过渡金属团簇的结构和芳香性的理论研究

在B3PW91/6-311+G(d)计算水平上, 计算并讨论了Ni₄Ti₂, [Ni₄Ti₂]²⁺, [Ni₄Ti₂]^2-与Ni₄Ti₄, [Ni₄Ti₄]²⁺, [Ni₄Ti₄]^2-团簇的几何结构和芳香性. 在构型优化过程中得到了Ni₄Ti₂(D_4h), [Ni₄Ti₂]²⁺(D_4h), [Ni₄Ti₂]^2-(D_4h)和Ni₄Ti₄(D_2h)4个稳定构型, 发现当引入上下2个Ti原子后, Ni₄环成为了平面正方形构型. 核无关化学位移(NICS)计算结果表明, Ni₄Ti₂(D_4h)与Ni₄Ti₄(D_2h)的NICS值为正, 而[Ni₄Ti₂]²⁺(D_4h)和[Ni₄Ti₂]^2-(D_4h)的NICS值为负, 且[Ni₄Ti₂]^2-(D_4h)的NICS值更负. 同时还发现, 由s与d轨道参与形成的反磁性环流是引起[Ni₄Ti₂]²⁺(D_4h)和[Ni₄Ti₂]^2-(D_4h)具有较大芳香性的主要原因; 其中Ti原子主要提供d_z²与s轨道, 而Ni原子主要利用其d_z²与d_x²-y²轨道形成正方形环, 它们之间构成了球状的d轨道环流, 且[Ni₄Ti₂]²⁺(D_4h)和[Ni₄Ti₂]^2-(D_4h)中还有非常明显的π轨道环流.     

异构体C36O的结构及其相对稳定性的理论研究

用abinitio方法和HF/STO-3G基组对Fullerenes的环氧衍生物C₃₆O所有可能的异构体进行非对称性限制下的结构优化,结合HF/6-31G水平上的单点能计算,确定其相对稳定性,得到等能量异构体的结构.张力分析的结果表明,C-O-C形成的三元环氧桥显著地削弱作用点附近C原子上所释放的张力,决定环氧位置选择性的关键因素不是碳笼上C原子的张力.对等能量异构体的红外光谱进行了理论预测.     

C70O2可能异构体的结构和电子光谱的理论研究

用AM1、PM3及INDO系列方法研究了C₇₀O₂可能异构体的结构和稳定性.在C₇₀O稳定构型的基础上,考察了C₇₀O₂的45种异构体.结果表明,两个O原子加在碳球极端处同一个六元环内不等价的6/6键上形成环氧结构的构型最稳定.在优化构型的基础上,进行电子光谱计算,并与C₇₀和C₇₀O进行了比较.     

C60O3的结构和电子光谱的理论研究

用INDO系列方法对C₆₀O₃的可能构型进行研究,结果表明:环氧结构邻近的6-6键易发生进一步的加成反应.其中3个氧原子加在同一个六元环的6-6边上,形成环氧结构最稳定的C₃v构型,第3个氧原子加在2个环氧结构相邻的六元环的6-6边上的C₂、C_s构型也相当稳定,C₂、C_s构型的部分¹³C NMR谱与实验吻合.C₆₀O₃可能有较好的反应活性,其电子光谱属于理论预测.     

中间体C60(CH3)-和产物C60(CH3)2的结构及产物

用INDO系列方法对C₆₀^2-与CH₃反应的中间体C₆₀(CH₃)^-进行理论研究,得到具有Cs对称性的构型。结果表明,CH₃加成到C₁₅上,将使与其相邻的双键碳(C₃₀)的电荷密度和自旋密度达极大值,故加成反应部位在C₃₀处;另外,C₁₅的对位C₁₂(或C₂₇)也较其它部位易于反应,且有两个反应场所,因而产物C₆₀(CH₃)₂可能为六元环上的1,2-加成和1,4-加成两种异构体的混合物。同时对两种加成产物的结构和电子光谱进行了理论研究,指认其电子跃迁,并讨论了其光谱红移的原因。     

C50(D5h)衍生物-异质富勒烯C48P2的分子行为理论研究

用半经验的AM1和MNDO方法以及密度泛函B3LYP/3-21G方法对C₅₀(D_5h)的衍生物C₄₈P₂的所有可能的异构体进行了系统的理论研究. 优化了稳定构型, 计算了生成热、HOMO-LUMO能级差、NICS值、红外光谱及电子光谱, 并与C₄₈X₂(X=B, N)的分子行为进行了比较. 计算结果表明: (1) C₄₈P₂的最稳定异构体是异构体C₄₈P₂-78, 该异构体对应于赤道位置六元环内的1,4-取代产物; (2) 决定C₄₈P₂异构体稳定性的主要因素是碳笼的张力, 而稳定性和芳香性之间没有明显的相关性; (3) 相对较稳定的C₄₈P₂异构体的HOMO-LUMO能级差比C₅₀的HOMO-LUMO能级差大; (4) 计算出的红外光谱以及电子光谱可以供实验参考; 计算出的NICS 值也可以用来表征C₄₈P₂各异构体. (5) C₄₈P₂与C₄₈X₂(X=B, N)具有相同的取代选择性规律及稳定性决定因素, 并且相对较稳定的异构体均具有比C₅₀本体大的HOMO-LUMO能级差.     

异质富勒烯C58BN的结构与光谱研究

用AM1、MNDO和INDO半经验方法研究了异质富勒烯C₅₈BN各异构体的结构、稳定性和电子光谱.所有这些半经验方法给出了相似的稳定性顺序.结果表明,在6-6位置取代的异构体是最稳定的,异构体的稳定性随杂原子间距离的增加而降低;与C₆₀相比,硼氮杂富勒烯C₅₈BN具有较低的前线轨道能级差、较小的电离势和较低的稳定化能.C₅₈BN很可能具有与C₆₀分子相似的反应活性,易发生亲核反应,但比C₆₀更易失去电子形成正离子.以AM₁优化构型为基础,利用INDO/CIS方法计算了各异构体的电子光谱.     

Electronic structures of dihedral (D5h, D5d, D6h, D6d) fullerenes

By means of our proposed method for Hückel theory calculation, we have calculated the electronic structures of dihedral (D_5h, D_5d, D_6h, D_6d) fullerences, which are generated from icosahedral C₂₀, C₆₀, C₈₀, C₁₈₀, C₂₄₀ and C₅₄₀, respectively. From the calculated results of 1224 fullerence molecules, certain rules on the stability and chemical reactivity have been drawn for such types of dihedral fullerenes.     

Ab initio and density function theory studies on NLi6 molecule: compared with CLi6 and OLi6 species

A wide variety of geometrical structures of NLi₆ molecule were studied using HF ab initio and BLYP-DFT techniques. Three stationary configurations which take D_4h, D_3d and D_2d configurations were obtained. Their equilibrium geometries and fundamental frequencies were calculated at HF and BLYP-DFT levels. Among the three stable states, the global minimum prefers D_3d configuration, which is different from those of CLi₆ and OLi₆. The D_3d isomer of NLi₆ is 3.43 and 28.45 kcal/mol lower in energy than the D_4h and D_2d ones in the DFT calculation, respectively. All calculations were performed with 6-31G* polarized split-valence basis set.     

乙硼烷离子和自由基结构的量子化学研究

用B₃LYP/6-311G(d,p)密度泛函方法对B₂H₅⁺阳离子和B₂H₅^·自由基的几何异构体的空间构型进行了优化,并在此基础上用QCISD(T)/6-311++G(3df,2p)偶合簇法进行了单点能计算和零点能校正.结果表明,B₂H₅⁺单态有2种稳定的几何构型(D_3h,C₁),其中C₁构型是新发现的.B₂H₅⁺三重态阳离子除已知C_s构型外,又发现两种稳定构型(C₁).对于B₂H₅^·自由基体系,共有4种异构体(包括两种新发现的构型C_s),其中,具有单桥结构的C_2v最稳定.用二级多体微扰理论和密度泛函方法对前人所认为稳定的B₂H₅⁺单态的C_2v构型进行了全优化,结果发现该构型始终具有一个虚频,不是稳定构型.对B₂H₅^-阴离子体系的单态和三重态进行的全优化,理论上得出单态时具有C_2v和C_s两种稳定构型,而三重态只有C_2v一种稳定构型.     

C80(Ⅰ,Ⅱ) and Sc2@C80(Ⅰ-Ⅲ):Production,Isolation and Spectrometric Studies

C₈₀ has seven structural isomers satisfying the isolated pentagon rule (IPR)^[1],however,only one isomer of C₈₀(D₂) was isolated and studied so far^[2]. In this study, we report the first successful isolation of multi-isomers of C₈₀ and C₈₀-based endohedral metallofullerenes. The new species were characterized by UV-Vis-NIR absorption spectroscopy, soot-extraction method, chromatographic retention time data and ¹³C NMR spectrometry (for C₈₀(Ⅱ)). It is suggested that C₈₀(Ⅱ) has a D_5d symmetry by the ¹³C NMR pattern (3×20; 2×10) and its long retention time in 5PYE column. For the three isomers of Sc₂@C₈₀,isomer Ⅲ has an extremely long retention time which suggests a D5d symmetry. On the contrary, isomer I has a very short retention time in 5PYE columnso it may have the most spherical I_h symmetry. Theoretically, Sc₂@C₈₀(I_h) is expected to have novel super-conductivity property as the A₃C₆₀ (A=K, Rb).     

Magnetic susceptibility of 1,1′,2,2′-tetramethylcobaltocene and 1,1′-diethylcobaltocene: Evidence for the dynamic Jahn-Teller effect

The magnetic susceptibility of 1,1′,2,2′-tetramethylcobaltocene, Co[C₅H₃(CH₃)₂]₂, and 1,1′-diethylcobaltocene, Co(C₅H₄C₂H₅)₂, has been studied between 0.99 and 296 K. The data are well reproduced by a calculation of the dynamic Jahn-Teller effect for the ²E_1g(a_1g²e_2g⁴e_1g) ground state of D_5d symmetry. A suitable set of parameter values is given by ζ = 100 cm⁻¹, δ = 150 cm⁻¹, k_JT = 0.40, κ = 0.70. The magnetism of cobaltocene, Co(C₅H₅)₂, may be described by parameter values of comparable magnitude. The results imply a significantly larger reduction of the spin-orbit coupling parameter ζ due to covalency than of the orbital reduction factor κ.     

Structures and energetics of C3H6S isomers: a Gaussian-3 ab initio study

Twenty-two isomers/conformers of C₃H₆S^+√ radical cations have been identified and their heats of formation (ΔH_f) at 0 and 298 K have been calculated using the Gaussian-3 (G3) method. Seven of these isomers are known and their ΔH_f data are available in the literature for comparison. The least energy isomer is found to be the thioacetone radical cation (4⁺) with C_2v symmetry. In contrast, the least energy C₃H₆O^+√ isomer is the 1-propen-2-ol radical cation. The G3 ΔH_f298 of 4⁺ is calculated to be 859.4 kJ mol⁻¹, ca. 38 kJ mol⁻¹ higher than the literature value, ≤821 kJ mol⁻¹. For allyl mercaptan radical cation (7⁺), the G3 ΔH_f298 is calculated to be 927.8 kJ mol⁻¹, also not in good agreement with the experimental estimate, 956 kJ mol⁻¹. Upon examining the experimental data and carrying out further calculations, it is shown that the G3 ΔH_f298 values for 4⁺ and 7⁺ should be more reliable than the compiled values. For the five remaining cations with available experimental thermal data, the agreement between the experimental and G3 results ranges from fair to excellent.

Cation CH₃CHSCH₂^+√ (10⁺) has the least energy among the eleven distonic radical cations identified. Their ΔH_f298 values range from 918 to 1151 kJ mol⁻¹. Nevertheless, only one of them, CH₂=SCH₂CH₂^+√ (12⁺), has been observed. Its G3 ΔH_f298 value is 980.9 kJ mol⁻¹, in fair agreement with the experimental result, 990 kJ mol⁻¹.

A couple of reactions involving C₃H₆S^+√ isomers CH₂=SCH₂CH₂^+√ (12⁺) and trimethylene sulfide radical cation (13⁺) have also been studied with the G3 method and the results are consistent with experimental findings.     

Size Dependence of Electronic Excitation Energy in Linear C2nH and C2n－1N

The geometries, bondings, and vibrational frequencies of C2nH (n = 3—9) and C2n-1N(n= 3—9) were in-vestigated by means of density functional theory (DFT). The vertical excitation energies for the X^2Ⅱ→^2Ⅱ transitions of C2nH(n= 3—9) and for the X2∑→^2Ⅱ and the X^2Ⅱ→^2Ⅱ transitions of C2n-1N (n= 3—9) have been calculated by the time-dependent density functional theory(TD-DFT) approach. On the basis of present calculations, the explicit expression for the wavelengths of the excitation energies in linear carbon chains is suggested, namely, λ0 = [1240. 6A/(2 √-3n 6 - √-3n 3）] (1 — Be^Cn), where A = 3. 24463, B =0. 90742, and C=0. 07862 for C2nH, and A=2. 94714, B=0. 83929, and C=0. 08539 for C2n-1N. In consid-eration of a comparison of the theory with the experiment, both the expressions are modified as λ1 = 0. 92 (λ0 100) and λ1 =0. 95(λ0-90) for C2nH and C2n-1N, respectively.     

Relative energies of isomers of C36F2

The symmetry unrestricted C₃₆F₂ isomers formed from fullerene C₃₆, the initial symmetry of which is C_6v, C_6h, or D_2d, have been extensively studied with semi-empirical (AM1 and PM3) calculations. Based on the relationship between the isomer's stability and the adding positions, three patterns of the adding sites of F₂ moiety in the additive reactions have been deducted. The results of the π-orbital axis vector (POAV) analysis indicate that the chemical reactivity of C₃₆ is the result of the high strain in the C₃₆ cage. But, in order to form stable compounds, the effects, which guide the F₂ moiety to select carbon atoms in the C₃₆ cage, are dominated by the conjugate effect in C₃₆F₂ system rather than the strain release in the C₃₆ cage.     

Electronic spectrum of jet-cooled cyanocyclopentadienyl radical

The D₁-D₀ electronic spectrum of jet-cooled cyanocyclopentadienyl (C₅H₄CN) radical, produced by excimer laser photolysis of 1,3-cyclopentadiene-1-carbonitrile (C₅H₅CN), was measured by laser-induced fluorescence (LIF). The LIF spectrum was identical to that of radicals produced by photolysis of phenyl isocyanate and o-chloroaniline, which had been assigned to phenyl nitrene. This result shows that the nascent radical product in the photolysis of o-chloroaniline and phenyl isocyanate is isomerized to C₅H₅CN and the final product of C₅H₄CN radical is derived via the second photolysis. The rotational contour of the 0-0 band of the C₅₄CN radical, at 27143 cm⁻¹ (368.3 nm), is also presented. The electronic transition is A-type and π electron transition, and the symmetry of both the ground and excited electronic state is ²B₁ (of the C_2v point group).