表面金属有机化学Ⅱ—SiO_2担载的三钌乙烯酮原子簇化合物[PPN]_2[Ru_3(CO)_9(CCO)]在CO加氢反应中的催化行为

本文分别通过三种不同的钌原子簇化合物[HRu_3(CO)_(11)]~-、Ru_6C(CO)_(17)和[Ru_3(CO)_9(CCO)~(2-)]制备了三种SiO_2担载型的钌催化剂,并研究了它们在CO加氢反应中的催化行为.结果表明,若和用[HRu_3(CO)_(11)]~-制备的催化剂相比较,用[Ru_3(CO)_9(CCO)]~(2-)制备的催化剂在CO加氢反应中显示了较高的活性.通过比较以上三种催化剂的催化行为以及所进行的红外和质谱表征,初步提出了用[Ru_3(CO)_9(CCO)]~(2-) 制备的催化剂上,CCO基团经脱羰基后可能转化成表面碳化物(Carbide),它是形成烃类产物的中间体.     

LiAl的电子与几何结构

应用平面波展开和第一原理赝势法研究了锂铝单晶的电子和几何结构,给出LiAl各种可能结构的能量～体积关系图以及相关的能带结构,电子态密度和电荷密度分布等各种性质变化关系.讨论了B32结构与其他结构电子键合性质的不同,指出B32结构之所以成为LiAl最稳定的结构是由于Al＿Al原子形成了类似于Si＿Si的共价键合.计算得到的能量最低的稳定结构与实验以及其它的理论计算结果一致.     

蛋白质的电子结构与活性关系——理论与计算方法

随着生物工程的发展,要求对蛋白质的电子结构与活性关系进行研究。而不加分割地对蛋白质作完整分子的量子化学计算,至今尚未见报导。其原因在于,未能找到合适的数值计算方法。本文报导了这方面的研究成果。假设一个蛋白质由N个氨基酸残基构成,其中有L对硫-硫键,每一个氨基酸残基有m_n个单元轨道,则整个蛋白质分子的分子轨道可以写成这些单元轨道的线性组合:     

Sb–C Bond Cleavage Reaction on a Triruthenium Cluster and the Formation of a Bridging Phenylacyl Unit

Syntheses and single crystal X-ray structures of an open triruthenium acyl carbonyl cluster [(C₆H₅)₂SbRu₃(COC₆H₅)(CO)₁₀] (1) and a simple triruthenium Ru₃(CO)₉[(C₆H₅)₂PCH₂P(C₆H₅)₂]Sb(C₆H₅)₃ (2) are reported. Formation of compound (1) at room temperature from [Ru₃(CO)₁₂] and [Sb(C₆H₅)₃] is unique, a similar reaction with Ru₃(CO)₁₀[(C₆H₅)₂PCH₂P(C₆H₅)₂] under identical conditions results in compound (2), with Sb(C₆H₅)₃ occupying an equatorial site. IR, ¹H, ¹³C NMR spectra of the compounds are reported. The X-ray crystal structure of (1) consist of 2 crystallography distinct molecules and shows Ru–Sb distances in the range: 2.6361(6)–2.6273(7) Å and Ru–Ru distances in the range: 2.8236(7)–2.9855(7) Å. Ru–O distances in the bridging carbonyl are: 2.137(4), 2.158(4) Å. The Sb–Ru–Ru angles in the two molecules of the asymmetric unit are in the range of 73.78(2)–77.52° indicating the puckered nature. Compound (2) has bond parameters comparable to those of Ru₃(CO)₁₀[(C₆H₅)₂PCH₂P(C₆H₅)₂]. The present study shows for the first time that the cleaving of Sb–C bond at room temperature is possible under non-ionic conditions, though there have been many instances of P–C and As–C bond cleavages reported previously.     

四苯基卟啉镍的电子结构及光谱研究

本文用INDO/CI方法计算了中位取代四苯基镍卟啉的电子结构与光谱。分子轨道能级表明平面型和垂直型的基态最高占有π轨道(a_(1w)和a_(2w))与次高占有轨道间有较大的能隙。计算的低激发态跃迁光谱表明,最低能量跃迁Q带和B带计算值与实验值符合较好,但N带与L带计算值偏高。算出的最低(nπ~*)跃迁出现在37000 cm~(-1)左右。     

推拉电子取代基对二茂铁衍生物性质及电子结构的影响

根据前线轨道理论分析３种具有推拉电子取代基的二茂铁衍生物循环伏安曲线、电子吸收光谱及光谱电化学行为，并给出了分子轨道能级图，实验结果表明，ＰⅡ有两对可逆氧化还原峰，Ｅ１、Ｅ２分别为０．３３、０．５９Ｖ，第一氧化态ＰⅡ＋￣（Ｄ—Ｆｃ￣＋—Ｒ）在６１３ｎｍ有强的ＬＭＣＴ（ｌｉｇａｎｄ－ｔｏ－ｍｅｔａｌ－ｃｈａｒｇｅ－ｔｒａｎｓｆｅｒ）带，是一种良好的光学特性氧化还原开关．ＰⅡ在３５４ｎｍ处出现强的ＬＭＣＴ带，ＰⅢ在３５６ｎｍ和３２０ｎｍ处分别出现强的ＬＭＣＴ和π→πＣＴ带，应具有较高的二阶分子极化系数，应当是较好的ＳＨＧ材料．     

杂原子取代卟啉的电子结构和光谱

用INDO/CI法计算了等电子氧杂、硫杂、氮杂卟啉的电子结构及低激发态电子跃迁.从前线轨道特征、电荷分布等与自由卟啉对比讨论了杂原子取代卟啉的电子结构.计算结果还预期了一些杂原子取代卟啉的低激发态电子跃迁光谱.     

镓原子链的结构稳定性和电子结构

The structural stabilities and electronic structures of Ga atomic chains are studied by the first-principles plane wave pseudopotential method based on the density functional theory. The present calculations show that gallium can form planar chains in linear-, zigzag- and ladder-form one-dimensional structures. The most stable one among the studied structures is the zigzag chain with a unit cell rather close to equilateral triangles with four nearest neighbors, and all the other structures are metastable. The relative structural stability, the energy bands and the charge densities are discussed based on the ab initio calculations and the Jahn-Teller effect.     

IR,Raman, and Surface‐enhanced Raman Spectroscopic Study on Triruthenium Dipyridylamide Diruthenium Nickel Dipyridylamide Family: Metal‐metal Bonding and Structures

We report the infrared, Raman, and surface‐enhanced Raman scattering (SERS) spectra of triruthenium dipyridylamido complexes and of diruthenium mixed nickel metal‐string complexes. From the results of analysis on the vibrational modes, we assigned their vibrational frequencies and structures. The infrared band at 323–326 cm^?1 is assigned to the Ru₃ asymmetric stretching mode for [Ru₃(dpa)₄Cl₂]^0–2+. In these complexes we observed no Raman band corresponding to the Ru₃ symmetric stretching mode although this mode is expected to have substantial Raman intensity. There is no frequency shift in the Ru₃ asymmetric stretching modes for the complexes with varied oxidational states. No splitting in Raman spectra for the pyridyl breathing line indicates similar bonding environment for both pyridyls in dpa^– , thus a delocalized structure in the [Ru₃]^6–8+ unit is proposed. For Ru₃(dpa)₄(CN)₂ complex series, we assign the infrared band at 302 cm^?1 to the Ru₃ asymmetric stretching mode and the weak Raman line at 285 cm^?1 to the Ru₃ symmetric stretching. Coordination to the strong axial ligand CN^– weakens the Ru‐Ru bonding. For the diruthenium nickel complex [Ru₂Ni(dpa)₄Cl₂]^0–1+, the diruthenium stretching mode ν_Ru‐Ru is assigned to the intense band at 327 and 333 cm^?1 in the Raman spectra for the neutral and oxidized forms, respectively. This implies a strong Ru‐Ru metal‐metal bonding.     

Ground State Structures,Electronic and Magnetic Properties of ScnFe (n=2–10) Clusters

The authors predict that the magnetic moment of the scandium clusters can not be efficiently enhanced with the encapsulation of Fe atom, which is different from previous works with Fe atom doped in B_n, Si_n, and Ge_n clusters. It was found that starting from n=6, the growth patterns of the ground state structures of the Sc_nFe clusters are dominated by the octahedron structures with Fe atom falling into the center of the host framework. The calculated results manifest that doping of the Fe atom contributes to strengthening the stabilities of the scandium framework. Maximum peaks are observed for clusters of n=3, 6 and 8 on the size dependence of the second‐order energy differences, implying that these clusters possess relatively higher stability. The HOMO‐LUMO gap of the Sc_nFe clusters exhibits an oscillational odd‐even character with the local peaks of n=4, 6 and 8. Especially, there is the largest oscillation of the gap with n=4 and 5. Additionally, the doped Fe atom exhibits the antiferromagnetic alignment at n=4, 5, 7 and 9. Also, the quench of the magnetic moments as n=6, 8 and 10 may be ascribed to the model of close‐shell electrons.     

Anderson型和Waugh型杂多阴离子的电子结构及其催化性能研究

使用SCC-DV-X_α法研究了两种杂多阴离子─(IMo₆O₂₄)^5-(Anderson型)和(NiMo₉O₃₂)^6-(Waugh型)的电子结构,并探讨了它们的催化性能。结果表明,两类杂多阴离子均具有催化活性,但不如Keggin结构强,(IMo₆O₂₄)^5-的催化活性中心是端氧O_t和中心八面体氧O_c.(NiMo₉O₂₄)^6-的催化活性中心是一配位端氧O_t、四配位中心氧和中心杂原子Ni,两类杂多阴离子中,二配位桥氧均不作为催化活性中心。     

Triruthenium dodecacarbonyl/triphenylphosphine catalyzed dehydrogenation of primary and secondary alcohols

Dehydrogenation of alcohols into aldehydes and ketones by Ru₃(CO)₁₂/PPh₃ based homogeneous catalysis has been investigated as an alternative for the classical Oppenauer oxidation. Several catalytic systems have been screened in the Oppenauer-like oxidation of alcohols. A systematic study of various combinations of Ru₃(CO)₁₂, mono- and bidentate ligands and hydride acceptors was performed to enable dehydrogenation of primary alcohols to stop at the aldehyde stage. Among many H-acceptors screened, diphenylacetylene (tolane) proved the most suitable judged from its smooth reduction. Electron rich and deficient analogues of tolane have been synthesized and, based on competition experiments between these H-acceptors, a tentative catalytic cycle for the Ru₃(CO)₁₂/PPh₃-catalyzed dehydrogenations has been proposed.     

FMBen（FM=Fe,Co,Ni;n=1-12）团簇结构和电子性质

采用密度泛函理论中的广义梯度近似对FMBen(FM=Fe,Co,Ni;n=1-12)团簇的几何构型进行优化,并对能量、频率和磁性进行了计算,同时考虑了电子的自旋多重度.结果表明,纯铍团簇的幻数是由电子的壳层模型确定,而FMBen团簇的幻数主要由几何效应来解释;掺杂铁磁性的过渡金属(Fe,Co,Ni)提高了纯团簇的稳定性.二阶能量差分表明FMBen(FM=Fe,Co,Ni)的幻数分别为5,10;5,10;4,10.通过对磁性质的研究发现掺杂不同的过渡金属时,磁矩出现了不同的变化规律.     

Dppm-substituted ruthenium clusters with capping sulfido and selenido ligands derived from thiourea, tetramethylthiourea and elemental selenium

Treatment of [Ru₃(CO)₁₀(μ-dppm)] (4) [dppm = bis(diphenylphosphido)methane] with tetramethylthiourea at 66 °C gave the previously reported dihydrido triruthenium cluster [Ru₃(μ-H)₂(μ₃-S)(CO)₇(μ-dppm)] (5) and the new compounds [Ru₃(μ₃-S)₂(CO)₇(μ-dppm)] (6), [Ru₃(μ₃-S)(CO)₇(μ₃-CO)(μ-dppm)] (7) and [Ru₃(μ₃-S){η¹-C(NMe₂)₂}(CO)₆(μ₃-CO)(μ-dppm)] (8) in 6%, 10%, 32% and 9% yields, respectively. Treatment of 4 with thiourea at the same temperature gave 5 and 7 in 30% and 10% yields, respectively. Compound 7 reacts further with tetramethylthiourea at 66 °C to yield 6 (30%) and a new compound [Ru₃(μ₃-S)₂{η¹-C(NMe₂)₂}(CO)₆(μ-dppm)] (9) (8%). Thermolysis of 8 in refluxing THF yields 7 in 55% yield. The reaction of 4 with selenium at 66 °C yields the new compounds [Ru₃(μ₃-Se)(CO)₇(μ₃-CO)(μ-dppm)] (10) and [Ru₃(μ₃-Se)(μ₃-η³-PhPCH₂PPh(C₆H₄)}(CO)₆(μ-CO)] (11) and the known compounds [Ru₃(μ-H)₂(μ₃-Se)(CO)₇(μ-dppm)] (12) and [Ru₄(μ₃-Se)₄(CO)₁₀(μ-dppm)] (13) in 29%, 5%, 2% and 5% yields, respectively. Treatment of 10 with tetramethylthiourea at 66 °C gives the mixed sulfur-selenium compounds [Ru₃(μ₃-S)(μ₃-Se)(CO)₇(μ-dppm)] (14) and [Ru₃(μ₃-S)(μ₃-Se){η¹-C(NMe₂)₂}(CO)₆(μ-dppm)] (15) in 38% and 10% yields, respectively. The single-crystal XRD structures of 6, 7, 8, 10, 14 and 15 are reported.     

FMBen(FM=Fe,Co, Ni; n=1-12)团簇结构和电子性质

采用密度泛函理论中的广义梯度近似对FMBen(FM=Fe, Co, Ni; n=1-12)团簇的几何构型进行优化, 并对能量、频率和磁性进行了计算, 同时考虑了电子的自旋多重度. 结果表明, 纯铍团簇的幻数是由电子的壳层模型确定, 而FMBen团簇的幻数主要由几何效应来解释; 掺杂铁磁性的过渡金属(Fe, Co, Ni)提高了纯团簇的稳定性. 二阶能量差分表明FMBen(FM=Fe, Co, Ni)的幻数分别为5, 10; 5, 10; 4, 10. 通过对磁性质的研究发现掺杂不同的过渡金属时, 磁矩出现了不同的变化规律.     

Electronic Structures and Spectra of the Bases and Base Pairs of Nucleic Acids

The present paper covers electronic structures and spectra of the bases and the base pairs of nucleic acids calculated by using the INDO/S method. For free bases we give the energy levels of ground states and transition energies of low-lying excited states and discuss the band characters. The results indicate that the calculated spectra are in good agreement with experimental values. On the other hand, our calculations for A-T and G-C pairs are very beneficial to understanding hydrogen bond properties of these pairs.     

X-ray Crystal Structures of Some Arene Oxides

Using a recently disclosed modification to the dimethyldioxirane method we have synthesized four arene monooxides and one trioxide in good to excellent yield. The X-ray crystal structures have been determined for all of these compounds. In the case of the chrysene trioxide the X-ray determination reveals that the structure is bent out of the plane.     

The Electronic and Magnetic Properties of a Few Transition-Metal Clusters

Using density functional theory we present a systematic study of the electronic and magnetic properties of various nickel clusters and two small bimetallic clusters, Ni _n Co _m and Ni _n Fe _m (n + m ≤ 6). A detail study of binding energy, magnetic moment and stability function of pure nickel clusters of nuclearity (N) 40–60 have been performed. We observe that the magic numbers occur at N = 43, 46, 49, 53, 55, and 58, which correspond to the most stable clusters. We find that, with increase in substitution of Co and Fe atoms in Ni cluster, while Ni _n Co _m becomes more stable, the Ni _n Fe _m clusters become less stable. The significant enhancement of average magnetic moment and suppression of local magnetic moment of nickel atoms are found in both clusters with increase in Co and Fe concentration.     

Studies on the Electronic Structures of the C_60, C_60H_60 and C_60F_60

The present paper represents the electronic structures of the cluster C60 and its derivatives C60H60 and C60F60 with FOOT-type of structure. On the basis of the total energies and molecular orbital energies from CNDO/2 calculations the clusters' stabilities, electronic configurations and charge distributions are discussed. The calculation results and discussion are very beneficial to understanding physical and chemical properties of the cluster C60 and its derivatives.     

Preparation of Titania Containing Mixed Oxides and Their Catalytic Activities

Titania containing catalysts were prepared by conventional procedures (coprecipitation, hydrogel kneading and titania precipitation) and a complexing-agent assisted sol-gel method. The effect of preparation methods on their properties and catalytic activities in the oxidation of olefins and decomposition of cumene hydroperoxide were examined. The sol-gel method gave the best dispersion of titania. In contrast, with the kneading and titania precipitation method, titania formed crystalline particles. The sol-gel catalysts are more effective for epoxydation of olefins because of the high dispersibility of Ti in them. However, the most active catalysts in the decomposition of cumene hydroperoxide are kneading ones.