Fe_(6-x)Al_x团簇的结构和磁性能

在密度泛函理论的BPW91水平上,对Fe6-xAlx团簇进行了结构优化,并将获得的最低能结构进行稳定性分析以及电子结构和磁性能的计算.计算结果表明,铁原子倾向团聚在一起并占据最高配位,Al原子则倾向分布在铁簇的周围尽最大可能地与Fe配位成键.Fe6-xAlx团簇的磁性随Al原子数目增加呈现下降趋势,自然轨道分析揭示Fe4s和Al3s与Fe3d之间的杂化是导致团簇磁矩下降的主要原因.     

过渡金属团簇Nbn、Con（n≤4）和NbxCoy（x＋y≤8）的芳香性

采用杂化密度泛函(DFF)方法优化了过渡金属纯团簇Nbn,Con(n≤4)和二元铌钴团簇NbxCoy(x+y≤8)的结构.并计算了较稳定结构的NICS(核独立化学位移)值,分析这些过渡金属团簇的成键情况,讨论不同轨道对各过渡金属团簇芳香性的贡献,发现在过渡金属团簇中,除了具有s,p轨道贡献的σ、π芳香性外,很重要的地d轨道的参与而形成的δ芳香性.     

过渡金属团簇Nbn、Con(n≤4)和NbxCoy(x+y≤8)的芳香性

采用杂化密度泛函(DFT)方法优化了过渡金属纯团簇Nbn, Con(n≤4)和二元铌钴团簇NbxCoy(x+y≤8)的结构, 并计算了较稳定结构的NICS(核独立化学位移)值, 分析这些过渡金属团簇的成键情况, 讨论不同轨道对各过渡金属团簇芳香性的贡献, 发现在过渡金属团簇中, 除了具有s、p轨道贡献的σ、π芳香性外, 很重要的地d轨道的参与而形成的δ芳香性.     

配体稳定的二元过渡金属团簇[PdAu8(PR3)8]2+(R=Me,OMe,H,F,Cl,CN)的量子化学理论研究

采用从头计算MP2方法和密度泛函理论方法,对过渡金属团簇[PdAu8(PR3)8]2+(R=Me,OMe,H,F,Cl,CN)的几何结构、电子结构以及团簇各组成部分之间的结合能进行了研究.MP2方法和SVWN局域泛函能够对团簇的结构给予准确的描述,而离域泛函BP86,PBE,BLYP和杂化泛函B3LYP则过高地估计了团簇的几何结构参数.电子结构研究表明Pd,Au原子通过d电子的成键作用构成团簇内核[PdAu8]2+,[PdAu8]2+与PR3配体则通过"σ给予/π反馈"模式成键.PR3配体与[PdAu8]2+的结合能够加强Pd-Au之间的成键作用,增大前线轨道能级间隙,从而提高团簇的稳定性.PR3配体中 R 基团供、吸电能力的变化对[PdAu8(PR3)8]2+结构的影响较小,但对[PdAu8]2+ -pR3结合能的影响较大.能量分析显示不同PR3与[PdAu8]2+之间具有相近的轨道作用能,与R基团供、吸电能力相关的非轨道作用能成为影响两者连接牢同程度的决定因素.     

(AB)_8(AB=BN, AlP, GaAs, InSb)团簇环状结构与性质的密度泛函理论研究

用杂化密度泛函B3LYP方法研究了(AB)8(AB=BN,AlP,GaAs,InSb)团簇环形结构的平衡几何构型、电子结构、振动特性以及极化率。计算结果表明,(AB)8团簇的双层环状结构中,每个A(B)原子都与3个B(A)原子成键,且Ⅴ族元素的原子比Ⅲ族元素的原子更接近团簇中心,(BN)8、(AlP)8、(GaAs)8、(InSb)8的平均极化率依次增大,IR和Raman谱峰发生红移。另外,讨论了热力学稳定性和动力学稳定性的变化。     

膦配体对金团簇[Au@Au8(PR3)8]3+(R=Me,OMe,H,F,Cl,CN)稳定化作用的理论研究

采用ab initio HF, MP2方法和密度泛函理论方法, 对具有D2h和D4d构型的膦配体稳定的过渡金属团簇[Au@Au8(PR3)8]3+(R=Me, OMe, H, F, Cl, CN)进行了几何结构、 电子结构及团簇稳定性等方面的研究. 计算表明, 与D2h构型相比, D4d构型更稳定, 两者能量相差约5~10 kJ/mol. SVWN局域泛函能够对团簇的几何结构给予较准确的描述, MP2方法对团簇的结构参数有所低估, 而离域和杂化泛函则过高地估计了团簇的结构参数. 电子结构分析表明, 中心Au原子与外围的Au原子之间通过 d 电子的成键作用构成团簇内核[Au@Au8]3+, [Au@Au8]3+与PR3配体则通过"σ给予/π反馈"模式成键. PR3配体与[Au@Au8]3+的结合能够加强内核-外围Au原子间的成键作用, 缩小外围Au原子在成键上的差异, 增大前线轨道能级间隙, 从而提高团簇的稳定性. PR3配体中R基团供、 吸电子能力的变化对[Au@Au8(PR3)8]3+结构影响较小, 但对[Au@Au8]3+-PR3结合能影响较大. 能量分析显示, 不同PR3配体与[Au@Au8]3+之间具有相近的轨道作用能, 与R基团供、 吸电子能力相关的非轨道作用能成为影响两者连接牢固程度的决定因素.     

Au12M (M=Na,Mg, Al,Si, P,S, Cl)团簇的结构、稳定性和电子性质

采用基于密度泛函理论的第一性原理方法系统地研究了Au12M(M=Na,Mg,Al,Si,P,S,Cl)团簇的结构、稳定性和电子性质.对团簇的平均结合能、镶嵌能、垂直离化势、最高占据分子轨道(HOMO)和最低未占据分子轨道(LUMO)的能级差、电荷布居分析、自然键轨道(NBO)进行了计算和讨论.对于Au12M(M=Na,Mg,Al)团簇,它们形成了内含M原子的最稳定的笼状结构.然而对于Au12M(M=Si,P,S,Cl)团簇,它们却形成了以M元素为顶点的稳定锥形结构.在这些团簇中发现Au12S团簇相对是最稳定的,这是由于Au12S团簇形成了稳定的满壳层的电子结构.自然电荷布居分析表明:对于所有的Au12M(M=Na,Mg,Al,Si,P,S,Cl)团簇电荷总是从Au原子转向M原子.自然键轨道和HOMO分析表明Au12M团簇中发生了Au原子的s-d轨道和M原子的p轨道间的杂化现象.     

TbSin(n=2-13)团簇的结构、电子及磁学性质

利用相对论密度泛函理论在广义梯度近似下研究TbSi_n (n=2-13)团簇的结构、稳定性、电子和磁学性质. 对团簇的平均结合能、离解能、电荷转移、最高占据分子轨道(HOMO)和最低未占据分子轨道(LUMO)的能级差、Mulliken 电荷分析和磁学性质进行了计算和讨论. TbSi_n团簇并没有像实验推测的那样在n=10形成嵌入式的结构. 我们推断电子亲和势的急剧变化不仅与嵌入式的结构有关, 而且与电子的固有稳定性相关.Mulliken 电荷分析表明电荷总是从Tb 原子转向Si 原子. 团簇的磁矩主要局域在Tb 原子的周围, 并且主要由f电子贡献, f 电子表现出局域性并且不参与化学成键. 以TbSi₁₀为例的分波态密度分析表明Tb与Si 原子间存在很强的sp轨道杂化.     

(AB)8(AB=BN，AlP，GaAs，InSb)团簇环状结构与性质的密度泛函理论研究

用杂化密度泛函B3LYP方法研究了(AB)₈(AB=BN，AlP，GaAs，InSb)团簇环形结构的平衡几何构型、电子结构、振动特性以及极化率。计算结果表明，(AB)₈团簇的双层环状结构中，每个A(B)原子都与3个B(A)原子成键，且Ⅴ族元素的原子比Ⅲ族元素的原子更接近团簇中心，(BN)₈、(AlP)₈、(GaAs)₈、(InSb)₈的平均极化率依次增大，IR和Raman谱峰发生红移。另外，讨论了热力学稳定性和动力学稳定性的变化。     

Pt_nNi_m（n＋m=7,n,m≠0）团簇结构稳定性与磁学性质

采用密度泛函理论（DFT）中的杂化密度泛函B3LYP方法在LANL2DZ基组水平上对PtnNim团簇的各种可能构型进行了几何结构全优化,得出了它们的基态构型,并对其稳定性和磁学性质进行了计算研究.研究结果表明：PtnNim团簇的基态结构都为立体结构,对称性较低,多重度较高,Pt5Ni2团簇的稳定性最好;从磁性上看,Pt...     

Spectra and excitation properties of (AlP)8: Effect of external electric fields

On the basis of density functional theory (DFT), the geometry and infrared spectrum of the (AlP)₈ cluster have been calculated under external electric fields (EEFs). In addition, on the basis of time-dependent DFT, the ultraviolet–visible absorption spectra, oscillator strengths, wavelengths, and hole–electron orbits of the first 20 excited states have been calculated. Under EEFs, the energy of (AlP)₈ gradually decreases, the dipole moment increases, and the molecular configuration significantly changes. In the infrared spectrum, the vibration frequency corresponding to the stretching vibration of the Al–P bond decreases, and a red shift occurs. With increasing EEF, the infrared spectrum splits and shows an obvious Stark effect; the ultraviolet absorption intensity is enhanced, and the molecular excitation energy decreases. Additionally, the excitation wavelength increases with increasing EEF. It is conclusively shown that the (AlP)₈ cluster is easily excited under an EEF. Separation of the holes and electrons of the (AlP)₈ cluster is obvious. Theoretical investigation of the spectra and excitation properties of (AlP)₈ is an important step toward a comprehensive understanding of the effects of EEFs on the molecular structure, stability, and dynamics.     

碳掺杂α-S_8的光学性质和弹性性质的第一性原理计算

采用第一性原理研究了C原子在光催化剂α-S8中掺杂后体系电子结构、能带结构、光学性质、弹性性质以及其各向异性的变化规律.结果表明C原子在α-S8中掺杂后新形成的C―S键键长变短、键的重叠布居数增加、电荷密度增加,表明新键的共价性变强.掺杂结构的带隙为2.64 eV,比纯α-S8的带隙小0.15 eV,表明掺杂后的结构导电性增强.掺杂结构的光吸收波长延长至650 nm左右,极大地提高了α-S8的光吸收效率.弹性性质计算表明C掺杂后α-S8的机械性能下降,但仍为脆性材料.各向异性的研究表明掺杂后的材料各向异性增强.     

CRYSTAL STRUCTURE OF （C8H8）Sm（2,4—C7H11）（THF）

<正> The crystal structure of (C8H8)Sm(2,4-C7H11)(THF)(2,4-C7H11 = 2, 4-dimethylpentadienyl) , Mr=421. 8, has been determined which, belongs to monoclinic space group P21 with a = 8. 682(3), 6 = 10. 968(3), c=9. 744(3) (?) ,β= 104.24(2)°, V = 899. 3(4)(?)3, Z = 2, Dc=1. 66g/cm3, μc=33. 2cm-1, F(000) = 422 and final R = 0. 041 for 2021 observed reflections with I≥ 2σ(I). The 2,4-dimethylpentadienyl group is in "U " conformation. The carbon-carbon bond distances within the pentadienyl ligand fall essentially in two sets. The average distance of external C - C bonds is shorter than that of the internal bonds.     

AlmN2 (m=1～8)团簇结构与稳定性的DFT研究

用密度泛函理论(DFT)的B3LYP方法，在6-31G*水平上对AlmN2(m=1～8) 团簇的几何构型、电子结构、振动频率和热力学性质进行了理论研究. 结果表明， AlmN2团簇的基态结构有两种基本构型， m≤2的结构是以N－N键为核心周围与Al原子相配位形成的; m >2的结构是由两个AlnN（n< m）分子碎片通过共用Al原子或Al－Al键相互结合形成的，这为较快找到AlmN2团簇基态结构提供了一条有效途径. 通过对基态结构能量二次差分的讨论，得到了m为偶数的AlmN2团簇比m为奇数的稳定.     

Structure and stability of B8 clusters

We investigated various isomers of B₈ clusters with ab initio (MP2) and density function theory (DFT) methods (B3LYP and B3PW91). Nineteen B₈ isomers were determined to be local minima on their potential energy hypersurfaces by the B3LYP, B3PW91, and MP2 methods. Fifteen of these structures are first reported. The most stable neutral B₈ cluster is the regular heptagon, with another boron atom at the center (D_7h, triplet), in agreement with results reported previously. The natural bond orbital (NBO) analysis and nucleus‐independent chemical shifts (NICS) further reveal that the most stable species have delocalized π bond and multicentered σ bonds and therefore exhibit multiple‐fold aromaticity. © 2004 Wiley Periodicals, Inc. Int J Quantum Chem, 2005     

Metal–Organic Frameworks (MOFs) of a Cubic Metal Cluster with Multicentered MnIMnI Bonds

MOFs with both multicentered metal–metal bonds and low‐oxidation‐state (LOS) metal ions have been underexplored hitherto. Here we report the first cubic [Mn^I₈] cluster‐based MOF ( 1 ) with multicentered Mn^I? Mn^I bonds and +1 oxidation state of manganese (Mn^I or Mn(I)), as is supported by single‐crystal structure determination, XPS analyses, and quantum chemical studies. Compound 1 possesses the shortest Mn^I? Mn^I bond of 2.372 Å. Theoretical studies with density functional theory (DFT) reveal extensive electron delocalization over the [Mn^I₈] cube. The 48 electrons in the [Mn^I₈] cube fully occupy half of the 3d‐based and the lowest 4s‐based bonding orbitals, with six electrons lying at the nonbonding 3d‐orbitals. This bonding feature renders so‐called cubic aromaticity. Magnetic properties measurements show that 1 is an antiferromagnet. This work is expected to inspire further investigation of cubic metal–metal bonding, MOF materials with LOS metals, and metalloaromatic theory.     

聚铝硅烷与聚碳硅烷共混先驱体制备SiC(Al)纤维

采用聚铝碳硅烷和聚碳硅烷共混制备含铝碳化硅的先驱体,并与直接合成得到的聚铝碳硅烷进行了比较.元素分析表明,共混法能够有效控制聚铝碳硅烷中的铝含量,且共混聚铝碳硅烷先驱体Si—H键含量更高.流变性能研究表明,共混获得的聚铝碳硅烷先驱体黏流活化能从255kJ/mol降至200kJ/mol,先驱体的可纺性提高,所以原纤维的平均直径从19μm降至12μm.预氧化后聚铝碳硅烷原纤维经1800℃一步烧成可得到致密的SiC(Al)纤维;XRD研究表明,纤维中的铝起到抑制碳化硅晶粒长大的作用.     

Antiferromagnetic Stabilization in the Ti8O12 Cluster

Using the evolutionary algorithm USPEX and DFT+U calculations, we predicted a high‐symmetry geometric structure of the bare Ti₈O₁₂ cluster composed of 8 Ti atoms forming a cube, in which O atoms are at midpoints of all of its edges, in excellent agreement with experimental results. Using natural bond orbital analysis, adaptive natural density partitioning algorithm, electron localization function, and partial charge plots, we find the origin of the particular stability of bare Ti₈O₁₂ cluster: unique chemical bonding where eight electrons of Ti atoms interacting with each other in antiferromagnetic fashion to lower the total energy of the system. The bare Ti₈O₁₂ is thus an unusual molecule stabilized by d‐orbital antiferromagnetic coupling.     

[Ca(NH2)2]n(n=1～5)团簇的密度泛函理论研究

用密度泛函理论(DFT)的杂化密度泛函B3LYP方法在6-31G*基组水平上对[Ca(NH2)2]n (n＝1～5)团簇各种可能的构型进行几何结构优化, 预测了各团簇的最稳定结构. 并对最稳定结构的振动特性、成键特性、电荷特性等进行了理论研究. 结果表明: 团簇易形成环状结构, 以金属Ca原子团簇作为骨架, NH2基结合在金属团簇骨架上, 并主要是Ca—N成键和Ca—Ca成键. 团簇中Ca—N键长为0.225～0.257 nm, Ca—Ca键长为0.312～0.354 nm, N—H键长为0.102～0.103 nm, H—N—H键角为102.9°～104.2°; 团簇中Ca原子的自然电荷在1.657e～1.720e之间, N原子的自然电荷在－1.543e～－1.592e之间, H原子的自然电荷在0.349e～0.367e之间, Ca原子和NH2基之间相互作用呈现较强的离子性;对比团簇和晶体的结构及IR谱表明, NH2基在团簇和晶体中的结构基本一致.     

Anomeric effects in the symmetrical and asymmetrical structures of triethylamine. Blue-shifts of the C-h stretching vibrations in complexed and protonated triethylamine

Quantum mechanical calculations using density functional theory with the hybrid B3LYP functional and the 6-31++G(d,p) basis set are performed on isolated triethylamine (TEA), its hydrogen-bond complex with phenol, and protonated TEA. The calculations include the optimized geometries and the results of a natural bond orbital (NBO) analysis (occupation of sigma* orbitals, hyperconjugative energies, and atomic charges). The harmonic frequencies of the C-H stretching vibrations of TEA are predicted at the same level of theory. Two stable structures are found for isolated TEA. In the most stable symmetrical structure (TEA-S), the three C-C bond lengths are equal and one of the C-H bond of each of the three CH2 groups is more elongated than the three other ones. In the asymmetrical structure (TEA-AS), one of the C-C bonds and two C-H bonds of two different CH2 groups are more elongated than the other ones. These structures result from the hyperconjugation of the N lone pair to the considered sigma*(C-H) orbitals (TEA-S) or to the sigma*(C-C) and sigma*(C-H) orbitals of the CH2 groups (TEA-AS). The formation of a OH...N hydrogen bond with phenol results in a decrease of the hyperconjugation, a contraction of the C-H bonds, and blue-shifts of 28-33 cm-1 (TEA-S) or 40-48 cm-1 (TEA-AS) of the nus(CH2) vibrations. The nu(CH3) vibrations are found to shift to a lesser extent. Cancellation of the lone pair reorganization in protonated TEA-S and TEA-AS results in large blue-shifts of the nu(CH2) vibrations, between 170 and 190 cm-1. Most importantly, in contrast with the blue-shifting hydrogen bonds involving C-H groups, the blue-shifts occurring at C-H groups not participating in hydrogen bond formation is mainly due to a reduction of the hyperconjugation and the resulting decrease in the occupation of the corresponding sigma*(C-H) orbitals. A linear correlation is established between the C-H distances and the occupation of the corresponding sigma*(C-H) orbitals in the CH2 groups.