双核Fe配合物[(η5-C5H4)C6H10(C4H3S)Fe(CO)2]2的合成和晶体结构

由侧链带有噻吩的环戊二烯基配体C5H5C6H10C4H3S与Fe(CO)5在二甲苯中加热回流,合成了1个新颖的四羰基二铁配合物[(η5-C5H4)C6H10(C4H3S)Fe(CO)2]2。通过元素分析、IR、1H NMR对其结构进行了表征,用X-射线单晶衍射确定了其结构。X-射线单晶衍射表明配合物中有2个桥羰基和2个端羰基,Fe-Fe的键长为0.25465(10)nm。     

吡啶配位的夹心型杂多阴离子{[Na(H2O)2]3[Ni(C5H5N)]3(AsW9O33)2}9-的结构及磁学性质

The pyridine coordinated sandwich-type heteropolytungstate Na7[Ni（H2O）6] { [Na（H2O）2]3[Ni（C5H5N）]3（AsW9O33）2}·28H2O was obtained by the reaction of Na2WO4·2H2O, NaAsO2 and pyridine with NiCl2·6H2O at pH =7.0 and characterized by elemental analysis, IR, UV-Vis,^1H NMR spectra and magnetic measurement. The structure of this heteropolytungstate was determined by X-ray diffraction analysis, which crystallized in triclinic system, space group P1 with a= 1.3153（9） nm, b= 1.7228（12） nm, c=2.6866（19） nm, a=74.130（11）°,β=78.032（12）°, γ = 73.179（12）° and Z= 2, R1 = 0.0604, wR2 = 0.0915 [I〉 2σ（I）]. Polyanion {[Na（H2O）2]3[Ni（C5H5N）]3（AsW9O33）2}^9- has approximately C3 symmetry, and three pyridine coordinated Ni（C5H5N）^2＋ and three Na（H2O）2^＋ are encapsulated between two AsW9O33^9- . Magnetic measurements show that central Ni3 unit in the polyanion exhibits ferromagnetic Ni-Ni exchange interactions （J=6.17 cm^-1）.     

新型取代基炔类分子的合成及其与B(C6F5)3的反应

合成了5种不同取代基的炔类化合物Mes2HSiC≡CPh(1,Mes=2,4,6-Me3C6H2)、[tBuC(NAr)2]GeC≡CPh(2,Ar=2,6-iPr2C6H3)、[PhC(NtBu)2]SnC≡CPPh2(3)、[HC(CMe)2(NAr)2]Sn C≡CPPh2(4)和[HC(CMe)2(NAr)2]ZnC≡CPPh2(5),研究了这些化合物与B(C6F5)3的反应.在与B(C6F5)3的反应中,1和2均发生1,1-碳硼化反应生成烯烃化合物(Ph)(Mes2HSi)C=C(C6F5)B(C6F5)2 (6)和{[tBuC(NAr)2]Ge}(Ph)C=C(C6F5)B(C6F5)2 (7), 7是一种GeⅡ/B松散Lewis酸碱对化合物;3~5则都发生B(C6F5)3与配体金属基的位置交换、进而配体金属基转换键合PPh2的反应,分别生成新颖的分子内双性离子炔烃化合物[PhC(NtBu)2]SnP(Ph2)C≡CB(C6F5)3 (8)、[HC(CMe)2(NAr)2]SnP(Ph2)C≡CB(C6F5)3(9)、[HC(CMe)2(NAr)2]ZnP(Ph2)C≡CB(C6F5)3 (10).文中还讨论了反应机理.     

新型层状磷酸铝[Al6P8O32][(C2H5)2NHCH2CH2NH3]2·[C2H5NH2CH2CH2NH2C2H5] 的合成、表征及其共模板作用

在溶剂热体系中,以N,N-二乙基乙二胺为结构导向剂,合成了Al/P为3/4的层状磷酸铝[Al6P8O32][(C2H5)2NHCH2CH2NH3]2·[C2H5NH2CH2CH2NH2C2H5]单晶,并通过X射线单晶衍射结构分析.XRD,ICP,元素分析,差热-热重分析等手段进行了表征.该化合物属单斜晶系,P2(1)/c空间群,晶胞参数:a=0.90945(2)nm,b=1.46424(4)nm,c=1.87572(5)nm,β=102.672(2)°,Z=4.其阴离子层由AlO4四面体和PO3(=O)四面体单元交替连接构成,形成四、六、八元环拓扑结构,无机层以ABAB方式堆积,两种质子化的有机胺分子N,N-二乙基乙二胺及其重排产物N,N′-二乙基乙二胺填充在层间.用分子动力学模拟方法,考察了标题化合物中有机胺与无机层间的相互作用,讨论了这两种有机胺的共模板作用.     

单茂钪催化剂（C5H5）Sc（CH2C6H4NMe2-o）2合成高顺式窄分布聚丁二烯

合成了6种单茂稀土催化剂Cp’LnR2(THF)n(其中,Cp’=C5H5,C5Me4SiMe3;R=CH2C6H4NMe2-o,CH2SiMe3;Ln=Sc,Y,Lu;n=0或1),并以[Ph3C][B(C6F5)4]为助催化剂,甲苯为溶剂,考察催化剂结构对丁二烯聚合活性,立体选择性,催化剂利用率以及聚合物分子量和分子量分布的影响.通过1H-NMR,13C-NMR,FTIR,GPC以及DSC对聚丁二烯进行表征,结果表明,当Cp’=C5H5,R=CH2C6H4NMe2-o,Ln=Sc,n=0时,催化剂(C5H5)Sc(CH2C6H4NMe2-o)2对丁二烯聚合活性最高,可达9600 kg-polymer/mol-Sc·h,催化剂利用率为45%,聚丁二烯顺-1,4结构含量在96%~98%之间,分子量分布窄,指数在1.3左右;以甲苯或氯苯作为聚合溶剂时,聚合活性最高,聚丁二烯分子量保持窄分布,在所有溶剂中聚丁二烯顺-1,4结构含量均达到96%以上;催化剂聚合活性随温度下降而降低,而聚合物分子量分布有变窄的趋势,温度对聚丁二烯立体选择性无明显影响;当[Bd]/[Sc]摩尔比从500增加到3000时,聚合反应1 min转化率均达到100%,聚丁二烯分子量呈可控线性增大,最高达44.6×104,且均保持聚合物窄分布.DSC谱图表明聚丁二烯Tg为-107℃,当升降温速率为10 K/min时,在-63℃和-8℃附近呈现出明显的冷结晶峰和熔融峰.     

B(C2H5)2q及其衍生物电子光谱性质的密度泛函理论研究

采用密度泛函理论(DFT)B3LYP、abinitioHF和单激发组态相互作用(CIS)等方法分别优化了有机配合物B(C2H5)2q及其衍生物的基态及最低激发单重态几何结构.用含时密度泛函理论(TD-DFT)对B(C2H5)2q及其衍生物的电子光谱进行了研究.发现该类物质是配体发光配合物,其发光源于8-羟基喹啉配体内π*     

新型镉配合物{[Cd2(C20H17N3O3F2)2（C8H4O4）2]·H2O}的合成及其晶体结构

以沙拉沙星为主要配体,对苯二甲酸为桥联配体,镉(Cd)为配位反应中心,利用水热法合成了新型配合物[Cd2(C20H17N3O3F2)2(C8H4O4)2].H2O(1),其结构经X-射线单晶衍射和元素分析表征。1属单斜晶系,空间群C2/c,晶胞参数a=19.994 1(8),b=11.166 6(3),c=22.561 4(8),β=95.826(3)°,V=5 011.2(3)3,Z=4,Dc=1.781 g.cm-3,R1=0.054 6,ωR2=0.099 5。1中每个Cd原子与一个沙拉沙星配体、三个对苯二甲酸以及一个游离的水分子配位,形成了具有无限伸展孔道结构的二维网络结构。     

金属配位聚合物[Mn2（C8H3NO6）2(C12H8N2)2]n的合成及其催化氧化性能

以5-硝基间苯二甲酸,1,10-邻菲啰啉,硫酸锰(MnSO4.H2O)为原料合成了一种结构新颖的金属配位聚合物——[Mn2(C8H3NO6)2(C12H8N2)2]n(1),其结构经IR,XRD,TG-DTG和元素分析表征。X-射线单晶衍射测试结果表明,1属三斜晶系,空间群Pī,晶胞参数a=10.060 2(1),b=14.343 5(2),c=14.663 7(2),α=104.052(1)°,β=102.633(1)°,γ=110.460(1)°,Mr=888.52,V=1 812.69(4)3,Z=2,Dc=1.628 g.cm-3,F(000)=900。以30%H2O2为氧化剂,初步研究了1在苯乙烯氧化反应中的催化氧化性能。     

[C6N2H18]2[Mo5O15(HPO4)2]·H2O的水热合成与结构表征

通过水热法合成了一个新化合物[C6N2H18]2[Mo5O15(HPO4)2]·H2O,并通过IR光谱、ICP、元素分析、差热与热重分析和X射线单晶衍射分析等手段进行了表征.结果表明,晶体属三方晶系,P3(2)21空间群,a=1.1231(1)nm,c=2.2802(5)nm,V=2.4911(7)nm3,Dx=2.835Mg/m3,Z=6,最后的一致性因子R=0.0227,wR=0.0675.阴离子中Mo5O15构成一环状结构,2个HPO4一个连在环的下方,一个连在环的上方,形成类似于“飞碟”状的结构,阳离子为2个质子化的四甲基乙二胺.     

新型双核配位聚合物Ni2（A`B`T`C`）（phen）2（H2O）4·4H2O的合成及其晶体结构

以A`B`T`C`(2,2’,3,3’-偶氮苯四甲酸)和Phen(邻啡啰啉)为配体,采用溶剂挥发法合成了一种新型双核配位聚合物Ni2(A`B`T`C`)(phen)2(H2O)4.4H2O(1),其结构经X-射线单晶衍射和元素分析表征。1属三斜晶系,空间群P-1,晶胞参数a=9.432(11),b=10.697(12),c=10.751(12),α=87.946(17)°,β=67.756(15)°,γ=76.085(16)°,V=972.6843,Z=12,Dc=4.740 mg.cm-3,μ=4.039 mm-1,F(000)=1 364,R1=0.042 5,ωR2=0.132 9。1中Ni(Ⅱ)与A`B`T`C中的两个羧基氧原子,两个H2O中的两个氧原子和phen中的两个氮原子配位,形成一个畸变的八面体几何构型。Ni(Ⅱ)经配体A`B`T`C桥联形成一维链,链与链之间又通过氢键堆积成三维超分子结构。     

Theoretical study of the molecular ions SiH−5 and SiH−3

Ab initio HF and Cl calculations were performed to determine the equilibrium geometry of SiH^?₅ and SiH^?₃, the barrier for internal rotation (SiH^?₅) and inversion (SiH^?₃) and the stability of SiH^?₅ and further to study the effect of electron correlation on reaction energies. The gaussian-type basis included d and f functions on Si and a p set on II. The D_3h structures of SiH^?₅ is lower in energy than the C_4v structure by 2.9(3.2) kcal/mol (corresponding HF results in parentheses). SiH^?₃ has C_3v structure, the inner-ion barrier computed is 26.2 (27.3) kcal/mol. SiH^?₅ turns out to be stable with respect to SiH₄ + H^? by 20.3 (13.8) kcal/mol, but it is unstable with respect to SiH^?₃ ← H₂ by 6.3 (5.6) kcal/mol. These results show that electron correlation has a small effect on barriers of inversion (SiH^?₃) or pseudorotation (SiH^?₅), but may have a pronounced effect on reaction energies even if all systems involved have closed shells. The correlation energy contributions are analyzed in terms of intrapair and interpair terms in order to get a better understanding of the influence of correlation on reaction and activation energies.     

Rydberg states of H4

Ab initio frozen core CEPA calculations have been performed in order to predict vertical energy levels and disccosiation energies for the Rydberg states of H₄ up to n_eff = 5. The electron correlation energies are analysed and discussed.     

Semiconductor-metal transition in Ti3O5

Ti₃O₅ shows a first-order phase transition from the monoclinic structure to the pseudobrookite structure at 448°K, at which temperature a magnetic susceptibility anomaly has been reported earlier in the literature. There is an electrical conductivity discontinuity accompanying the phase transition. Incorporation of Fe stabilizes the high-temperature phase of Ti₃O₅; while with 2% Fe the transition temperature and enthalpy change are lowered, with 5% Fe there is no transition. Mössbauer spectra of 2% Fe-doped Ti₃O₅ are similar below and above the transition temperature and show no evidence for magnetic ordering in the low-temperature phase. These results are compared to the VO₂ transition.     

Thermal studies on the electrical conductivity of some (CnH2n+1NH3)2CuCl4 (n = 1,2) and (CH2)(CH3)2CuCl4 complexes

The electrical conductivities of the compounds (CH₃NH₃)₂CuCl₄, (C₂H₅NH₃)₂CuCl₄ and (CH₂)₂(NH₃)₂CuCl₄ were measured in the temperature range which includes their structural phase transition. The values of the activation energies as calculated from the Arrhenius equation are reported. Confirmation of the phase transition temperatures is carried out using differential thermal analysis in the same temperature range as the conductivity measurements.     

Density functional calculations of Ni5 and Ni6 clusters

Density functional calculations on the electronic structure and magnetic properties of Ni₅ and Ni₆ clusters are presented in this work. The geometry and spin state of clusters are optimized for several starting symmetries. Moreover, those calculations are followed by a vibrational analysis to discriminate between real minima and saddle-points on the potential energy surface of clusters. Equilibrium geometries, electronic configurations, binding energies, magnetic moments, and harmonic frequencies of stable Ni₅ and Ni₆ clusters are reported.     

Potential curves for dissociative electron attachment of CFCl3

Ab initio MRD CI potential curves are reported for CFCI₃ and CFCI₃ and the results are seen to give quantitative support to a recent interpretation of the dissociative electron attachment phenomenon in halocarbons, including the fact that in CFCl₃ itself such processes occur with essentially zero electron impact energies. Calculated vertical IP and transition energy results also found fit in quite well with corresponding measured values.     

A study of electronic structure of SbCl5.L and SnCl4.L2 complexes by the PM3 method

Electronic structures of SbCl₅.L and SnCl₄.L₂ complexes were studied by the semiempirical PM3 method. The results were compared with the data from ³⁵Cl NQR and ¹²¹Sb NQR studies and Mössbauer spectra.

A good correlation was obtained between the calculated and experimental values of quadrupole coupling constants. The calculated energies of the donor-acceptor bond formation were compared with the degree of electron density transfer. The derived correlation dependences between the above two parameters suggest different properties for cis and trans complexes.     

A study of electronic structure of SbCl5.L and SnCl4.L2 complexes by the PM3 method

Electronic structures of SbCl₅.L and SnCl₄.L₂ complexes were studied by the semiempirical PM3 method. The results were compared with the data from ³⁵Cl NQR and ¹²¹Sb NQR studies and Mössbauer spectra.

A good correlation was obtained between the calculated and experimental values of quadrupole coupling constants. The calculated energies of the donor-acceptor bond formation were compared with the degree of electron density transfer. The derived correlation dependences between the above two parameters suggest different properties for cis and trans complexes.     

Electronic structure of UF5

Non-relativistic and relativistic self-consistent Hartree—Fock—Slater and Dirac—Slater models have been used to calculate one-electron energy levels and ionization energies for UF₅. The calculations were performed in an assumed structure of C_4v symmetry with the uranium atom at the center of mass of the molecule. The spacing and level ordering are compared with earlier results obtained with the MS Xα method using the muffin-tin approximation. Connections with the multi-photon isotope separation scheme of UF₆ are discussed.     

The molecular structures of H2Os3(CO)10, H(SC2H5)Os3(CO)10 and (OCH3)2Os3(CO)10

X-ray crystallographic analyses of H₂Os₃(CO)₁₀, H(SC₂H₅)Os₃(CO)₁₀ and (OCH₃)₂Os₃(CO)₁₀ are reported. Although hydrogen atom positions have not been located, the essential isostructural nature of the three commplexes establishes the hydride ligands as bridging two metal atoms, separated by 2.670 Å, with a formal bond order of two; the bridging hydrido- and thiolato-ligands span an osmium---osmium bond of length 2.863 Å and formal bond order one; the two μ-methoxy ligands bridge two metal atoms separated by 3.078 Å which, by simple 18 electron rule counting, has a metal---metal bond order of zero. Some general comments are made on the structures of polynuclear transition metal carbonyls.