Étude lcao-mo-cndo/2 des liaisons po et no dans des composés X3PO ET X3NO

The authors have studied the electronic structure of X₃PO and X₃NO compounds (with X = F, Cl, CH₃), using the semi-empirical CNDO/2 method. All the calculations have been made with and without 3d functions on the phosphorus atom. The comparison between the calculated and experimental values, especially in the case of bond length, dipole moment, and orbital level order, shows the influence of the 3d orbitals in the PO bond, which contains a sigma donation P → O and a pπ(O)-dπ(P) back bonding. The NO bond has sigma character in trimethylamine oxide, but is partially a double bond in trifluoramine oxide.     

Local structure in solid solutions of stabilised zirconia with actinide dioxides (UO2, NpO2)

The local structure of (Zr,Lu,U)O_2−x and (Zr,Y,Np)O_2−x solid solutions has been investigated by extended X-ray absorption fine structure (EXAFS). Samples were prepared by mixing reactive (Zr,Lu)O_2−x and (Zr,Y)O_2−x precursor materials with the actinide oxide powders, respectively. Sintering at 1600 °C in Ar/H₂ yields a fluorite structure with U(IV) and Np(IV). As typical for stabilised zirconia the metal-oxygen and metal-metal distances are characteristic for the different metal ions. The bond lengths increase with actinide concentration, whereas highest adaptation to the bulk stabilised zirconia structure was observed for UO and NpO bonds. The ZrO bond shows only a slight increase from 2.14 Å at 6 mol% actinide to 2.18 Å at infinite dilution in UO₂ and NpO₂. The short interatomic distance between Zr and the surrounding oxygen and metal atoms indicate a low relaxation of Zr with respect to the bulk structure, i.e. a strong Pauling behaviour.     

五配位铁硫化合物(Et4N)4〔Fe2(S,X-C6H4-o)4〕的合成与晶体结构

利用无水FeCl与双齿配体Na_2BDT或Na_2MP(Na_2S,X-C,H_4-o_2:X=S,BDT;X=O,MP)在乙醇溶液中反应,然后加入沉淀剂Et_4NBr,可以得到双核铁硫化合物(Et_4N)_2[Fe_(S,X-CH_4-o)_4](1,X=S;2,X=0)。它们分别具有以双硫或双氧桥联起来的五配位扭曲三角双锥构型的铁原子。分子为心对称,核心Fe_2X_2~(2+)为平面。每个铁原子上的二个苯环平面A和B相互近于平行(1,二面角10.1°)或近于垂直(2,二面角100.2°);但铁原子与XSCC平面非共面。Fe原子离平面0.05～0.5A。2是第一个以双齿配位的双氧桥铁硫化合物,它既含有桥基氧原子又具有端基氧原子,对研究含氧配位的铁原子周围环境,为模拟固氧酶中的“P簇”,有一定意义。     

Syntheses, structure characterisation and X-ray studies of some mono, di- and tri-substituted cluster complexes of Ru3(CO)12 substituted by bulky fluorinated phosphine ligands

Five trinuclear substituted complexes of the type Ru₃(CO)₁₁L, Ru₃(CO)₁₀L₂ and Ru₃(CO)₉L₃ were synthesised by the reaction of Ru₃(CO)₁₂ with fluorine substituted phosphine ligands, {P(C₆H₄F-m)₃ and P(C₆H₄F-p)₃}, using the radical anion catalysed method. The structures of the resulting clusters were elucidated by means of elemental analyses and spectroscopic methods, which included IR, ¹H, ¹³C and ³¹P NMR spectroscopy. X-ray crystallographic studies of four of the complexes were carried out. In all the complexes, the ligand occupies an equatorial position due to steric reasons, and coordination of the ligand is observed only at the phosphorus atom. In the two monosubstituted complexes, Ru₃(CO)₁₁P(C₆H₄F-m)₃ and Ru₃(CO)₁₁P(C₆H₄F-p)₃, the effect of substitution resulted in an increase in the Ru-Ru distances. Out of the three Ru-Ru bonds, the one which is cis to the ligand is noticeably longer than the other two. The asymmetric unit of the disubstituted complex Ru₃(CO)₁₀{P(C₆H₄F-p)₃}₂ is composed of two molecules, A and B. As expected, the two phosphorus ligands are equatorially bonded to two different ruthenium atoms. The asymmetric unit of the trisubstituted complex is composed of one molecule of Ru₃(CO)₉{P(C₆H₄F-m)₃}₃ and one disordered solvent molecule. The structure consists of one triangular ruthenium complex in which each of the phosphorus ligands is equatorially bonded to three different ruthenium atoms. In the structure, disorder of the fluorine atoms is observed. Bond parameters, especially bond lengths and bond angles, are correlated to the structure and also are compared with the literature data of similar compounds.     

Theoretical Studies of Inorganic Compounds. 341) Energy Decomposition Analysis of E–E Bonding in Planar and Perpendicular X2E−EX2 (E = B,Al, Ga,In, Tl; X = H,F, Cl,Br, I)

The nature of E–E bonding in group 13 compounds X₂E–EX₂ (E = B, Al, Ga, In, Tl; X = H, F, Cl, Br, I) has been investigated by means of an energy decomposition analysis (EDA) at the BP86/TZ2P level of theory. The calculated equilibrium geometries of all molecules B₂X₄?Tl₂X₄ have a perpendicular (D_2d) geometry. The largest energy barriers for rotation about the E‐E bond are predicted for the hydrogen species B₂H₄?Tl₂H₄. The EDA shows that the rotational barriers of B₂X₄?Tl₂X₄ may not be used for an estimate of the hyperconjugative strength in the D_2d structures except for the tetrahydrides. The values for the planar (D_2h) transition states reveals that π conjugation of the halogen lone‐pair electrons stabilizes the transition states. The bonding analysis shows that hyperconjugation in B₂I₄ is stronger than in B₂H₄ although the latter compound has a higher rotational barrier than the former. In B₂F₄, hyperconjugative stabilization of the perpendicular structure and conjugative stabilization of the planar structure nearly cancel each other yielding a nearly vanishing rotational barrier. The heavier analogues Al₂X₄?Tl₂X₄ have low rotational barriers and rather weak hyperconjugative interactions. The larger rotational barriers of the hydrogen systems Al₂H₄?Tl₂H₄ compared with the tetrahalogen compounds is explained with the cooperation of the relatively large hyperconjugation in the perpendicular form and the relatively weak conjugation in the planar transition structures. The EDA also indicates that the electrostatic (ΔE_elstat) and molecular orbital (ΔE_orb) components of the E–E bonding are similar in magnitude.Thecalculated B‐B bond dissociation energies of B₂X₄ (D_e = 93.0–108.4 kcal/mol) show that the bonds are rather strong. The heavier analogues Al₂X₄?Tl₂X₄ have weaker bonds (D_e = 16.6–61.7 kcal/mol). In general, the X₂E‐EX₂ bond dissociation energies follow the trend for atoms E: B ? Al > Ga > In > Tl and for atoms X: H > F > Cl > I.     

A CNDO/2 investigation of the CH3/CF3 substitution effect

The variation of the A-C bond lengths with substitution of methyl by perfluoromethyl in molecules of the kind A(CH₃ )_n is investigated using the CNDO/2 method. Calculations were performed with A as fluorine, oxygen, nitrogen, sulphur and phosphorous and n = 1, 2 or 3. The variation of the A-C bond length can be explained qualitatively by combining two effects, (1) changes in the covalent bond order and (2) changes in the ionic bond strength. While the covalent bond order decreases in all cases, the extent of the decrease depending largely on the electronegativity of A, the ionic bond order increases for fluorine, oxygen, nitrogen and sulphur and decreases in the case of phosphorous. The variations in the ionic bond strength are found to depend on the electronegativity of A as well as on the number of substituted methyl groups.     

Approach to thermal properties and electronic polarizability from average single bond strength in ZnOBi2O3B2O3 glasses

The glass transition temperature (T_g), density, refractive index, Raman scattering spectra, and X-ray photoelectron spectra (XPS) for xZnO-yBi₂O₃-zB₂O₃ glasses (x=10-65, y=10-50, z=25-60 mol%) are measured to clarify the bonding and structure features of the glasses with large amounts of ZnO. The average electronic polarizability of oxide ions (α_O2−) and optical basicity (Λ) of the glasses estimated using Lorentz-Lorenz equation increase with increasing ZnO or Bi₂O₃ content, giving the values of α_O2−=1.963 Å³ and Λ=0.819 for 60ZnO-10Bi₂O₃-30B₂O₃ glass. The formation of BOBi and BOZn bridging bonds in the glass structure is suggested from Raman and XPS spectra. The average single bond strength (B_MO) proposed by Dimitrov and Komatsu is applied to the glasses and is calculated using single bond strengths of 150.6 kJ/mol for ZnO bonds in ZnO₄ groups, 102.5 kJ/mol for BiO bonds in BiO₆ groups, 498 kJ/mol for BO bonds in BO₃ groups, and 373 kJ/mol for BO bonds in BO₄ groups. Good correlations are observed between T_g and B_MO, Λ and B_MO, and T_g and Λ, proposing that the average single bond strength is a good parameter for understanding thermal and optical properties of ZnOBi₂O₃B₂O₃ glasses.     

Electronic interactions in 1-ethynyl-2-phenyltetramethyldisilanes HCCSiMe2SiMe2C6H4X

1-Ethynyl-2-phenyltetramethyldisilanes HCCSiMe₂SiMe₂C₆H₄X [X = NMe₂ (1), H (2), CH₃ (3), Br (4), CF₃ (5)] are accessible from ClSiMe₂SiMe₂Cl, BrMgC₆H₄X and HCCMgBr in a two step Grignard reaction. The crystal structure of 1 as determined by single crystal X-ray crystallography exhibits a nearly planar PhNMe₂ moiety and an unusual gauche array of the phenyl and the acetylene group with respect to rotation around the Si-Si bond. Full geometry optimization (B3LYP/6-31+G^∗∗) of the gas phase structures of 1-5 affords minima for the gauche and the anti rotational isomers, both being very close in energy with a rotational barrier of only 3-5 kJ/mol. Experimental and calculated (time-dependent DFT B3LYP/TZVP) UV absorption data of 1-5 show pronounced electronic interactions of the HCC- and the C₆H₄X π-systems with the central Si-Si bond.     

Structure and reactivity of derivatives of dihalogenomethyl indium(III) halides, X2InCHX2 (X = Cl, Br, I)

The reactions of indium monohalides, InX with haloforms, CHX₃, in 1,4-dioxane (diox), produce the dioxane adducts of dihalogeno-dihalogenomethyl-indium(III), X₂In(diox)_nCHX₂ (X = Cl, Br, n = 1; X = I, n = 2) compounds. The ionic derivative [(C₂H₅)₄N] [Cl₃InCHCl₂] was prepared and its crystal structure determined by X-ray means. The reactions of the X₂In(diox)_nCHX₂ compounds are significantly different from those of the related X₂InCH₂X compounds. The dihalogenomethyl derivatives react with strong electrophiles suggesting dihalogenomethyl substituents of mild nucleophilic character, while the carbon atoms in the halogenomethyl derivatives are electrophilic.     

Analysis of competing bonding parameters. Part 2. The structure of halosilanes and halogermanes (MH4−nXn,n=1–4; M=Si,Ge; X=F,Cl, Br)

A qualitative rationalization of bonding patterns in halosilanes and halogermanes (MH_4−nX_n, n=1–4; M=Si, Ge; X=F, Cl, Br) is presented. Geometrical and bonding properties in these molecules are discussed on the basis of ab initio molecular orbital calculations employing the natural bond orbital population analysis. The results have been compared with data derived previously for halomethanes. Differences in the n-dependence of the M–Cl and M–Br bond lengths for M=C, Si, Ge are explained by a significant reduction in the closed-shell repulsion between the halide atoms. As M gets larger, a continuous decrease in the X–M–X bond angle is observed. Small bond angles (for n=2, 3) are favoured by the p-rich M orbitals in the M–X bonds. They are opposed, however, by the X⋯X repulsion. As M gets larger, the X⋯X separation for a given bond angle increases. A reduction in the X–M–X bond angle is therefore accomplished without overcompensation due to the X⋯X repulsion energy. The variation in the charge density at M as a function of n has been rationalized by differences in the electronegativity of the terminal atoms H and X. Dipole moments have been computed for the molecules in the series. As in the fluoromethanes, a maximum in the dipole moments at n=2 is explained by a combination of geometric and electronic properties unique to the fluoro-compounds. These are, an n-independent charge density at the F sites and a significant decrease in the M–F bond distance as n increases.     

N8H8环状异构体的结构与稳定性的理论研究

采用密度泛函理论的B3LYP方法在6-311＋＋G**基组水平上对N₈H₈氮氢环状化合物可能存在的构型进行了几何优化, 得到74种稳定异构体, 应用自然键轨道理论NBO和分子中的原子理论AIM分析了这些化合物成键特征和相对稳定性, G3MP2方法计算了各异构体的能量及生成热. 研究结果表明: N原子孤对电子到相邻的氮氮键的超共轭作用是影响氮氮键长变化的主要因素; N₈H₈环状异构体的稳定性顺序为: 六元环＞七元环＞八元环, 五元环＞三元环＞四元环, 六元环是这些N₈H₈环状异构体中最稳定的, 最不稳定的是四元环, G19是所有环状异构体中能量最低的; M3能量最高, 稳定性最差, A7密度最大.     

The comparison of thermal stability of some hydrofluoroethers and hydrofluoropolyethers

The thermal stability of representative hydrofluoropolyether (HFPE) and hydrofluoroether (HFE) compounds has been evaluated. The observed stability order appears to be correlated with the nature of the hydrogenated chain ends; in particular, molecules having fully hydrogenated chain ends (OCH₃ and OC₂H₅) show a significantly lower stability compared with the OCF₂H terminated compounds. The main degradation products suggest, however, that the same primary reaction is responsible for the decomposition of all the compounds examined; this reaction involves the fragmentation of the R_fOC_xH_yF_z bond with fluorine transfer between the two carbon atoms close to the oxygen, leading to the formation of a hydrofluorocarbon C_xH_yF_(z+1) and an acyl fluoride or a ketone.     

Porous framework of T2[Fe(CN)6]·xH2O with T=Co, Ni, Cu, Zn, and H2 storage

The materials under study were prepared from aqueous solutions of ferrocyanic acid and salts of the involved transition metals and their crystal structure solved and refined from X-ray powder diffraction data. Complementary information from thermogravimetric, infrared and Mössbauer data was also used for the structural study. Three different crystal structures were found: hexagonal (P-3) for Zn with the zinc atom coordinated to three N ends of CN groups plus a water molecule, cubic (Pm-3m) for Ni and Cu, and monoclinic (P2₁/m) for Co. For Ni and Cu the obtained solids have an open channel framework related to 50% of vacancies for the building unit, [Fe(CN)₆]. In the as-synthesized material the framework free volume is occupied by coordinated and hydrogen-bonded water molecules. These of hexacyanoferrates (II) have received certain attention as prototype of materials for the hydrogen storage. In the anhydrous phase of Ni and Cu, 50% of the metal (T) coordination sites, located at the cavities surface, will be available to interact with the hydrogen molecule. However, when the crystal waters are removed the porous frameworks collapse as it is suggested by H₂ and CO₂ adsorption data. For Co, a structure of stacked layers was found where the cobalt atoms have both tetrahedral and octahedral coordination. The layers remain together through a network of hydrogen-bonding interactions between coordinated and weakly bonded water molecules. No H₂ adsorption was observed in the anhydrous phase of Co. For Zn, the porous framework remains stable on the water removal but with a system of narrow channels and a small available volume, also inaccessible to H₂.     

Recherche d'une description structurale des de´compositions endothermique Solide 1 → Solide 2 + gaz. I. Structure cristalline de l'oxalate de baryum 2BaC2O4, H2O

2BaC₂O₄ · H₂O (M = 468.73) is triclinic, space group P1, with a = 9.312(1) A?, b = 9.649(1) A?, c = 6.188(1) A?, α = 90.13(2)°, β = 95.36(2)°, γ = 125.18(2)°, Z = 2, D_m = 3.48; C_x = 3.51g · cm^?3. The position of the Ba atom was determined from a Patterson function. A subsequent Fourier synthesis clearly revealed the position of all C and O atoms in the structure. Refinement of the MoKα diffractometer data by a least-squares method using full matrix gave R = 0.065. The structure presents two remarkable characteristics: (a) We distinguish two types of (C₂O₄)^2? ions. The first are planar, the second are notably separated from the plane configuration (deviation = 30°); this deformation is of a steric origin. (b) The water molecules are located in channels parallel to [001]. They enter in the coordination of one of the Ba²⁺ ions but do not exchange any strong hydrogen bond with oxygen atoms which surround them.     

Mise en évidence de l'entité Sb2F4O dans un composé d'addition moléculaire avec l'urée étude structurale de [(NH2)2CO]2,Sb2F4O

The X-ray structure determination of [NH₂)₂CO]₂ · Sb₂F₄O shows the existence of linked units urea-Sb₂F₄O which show the Sb₂F₄O entity, not yet known. Crystal structure was solved with a singlecrystal X-ray diffraction study (the final R value is 0.046). The Sb₂F₄O unit is composed of a symmetric and short SbOSb bridge, and of four fluorine atoms, two being bonded to each antimony atom and situated in trans position relative to the SbOSb bridge. The bridge bond strength is assigned to a pπdπ overlap.     

Syntheses and crystal structures of [Mg(HF)2](SbF6)2 and [Ca(HF)2](SbF6)2: new examples of HF acting as a ligand to metal centres

[Mg(HF)₂](SbF₆)₂ and [Ca(HF)₂](SbF₆)₂ monocrystals were grown from the corresponding hexafluoroantimonates(V) dissolved in anhydrous hydrogen fluoride. [Mg(HF)₂](SbF₆)₂ crystallizes in the space group Pnma (no. 62) with a=1249.1(4) pm, b=1230.2(4) pm, c=699.1(2) pm, V=1.0742(6) nm³, Z=4. Magnesium is octahedrally coordinated by six fluorine atoms from which two belong to two HF molecules. The structure can be represented by alternating rows of magnesium and antimony atoms running parallel to the c-axis. Magnesium atoms are connected by cis bridging Sb(2)F₆ units along the a-axis and by trans bridging Sb(1)F₆ units along the b-axis. In this way a three-dimensional network is formed.[Ca(HF)₂](SbF₆)₂ crystallizes in the space group P2₁/n (no. 14) with a=935.2(3) pm, b=1088.7(3) pm, c=1104.8(3) pm, β=106.697(5)°, V=1.0774(5) nm³, Z=4. The coordination sphere around the calcium atom consists of eight fluorine atoms which define the vertices of an Archimedean antiprism. The two HF molecules directly coordinate the calcium atom and their fluorine atoms are placed in the corners of different square faces of the Archimedean antiprism. The Ca-F(HF) distances are shorter than the Ca-F(Sb) distances. The Sb(1)F₆ and Sb(2)F₆ groups have four equatorial bridging fluorine atoms, while the Sb(3)F₆ groups have only two bridging trans F ligands. The Ca atoms in the [−1,0,1] plane are connected by equatorial F ligands of Sb(1)F₆ and Sb(2)F₆ units, forming a [Ca(SbF₆)⁺]_n layer. These layers are connected by trans bridging Sb(3)F₆ groups. HF molecules occupy the space between these layers and additionally contribute to the connection between the layers by hydrogen bonding.     

Effect of the bridging ligands on the CO stretching force constants of the compounds Co2(CO)6(μ-Y)2 and Fe2(CO)6(μ-X)2 (where Y = CO,P, As,CR and X = S,SR, Se,PRR′, Br,I)

The molecular structures of (C₅H₅)₂V and (C₅H₅)₂Cr have been determined by gas phase electron diffraction. The best agreement between calculated and experimental curves is obtained for models with eclipsed C₅H₅ rings (symmetry D_5h), but models with staggered rings (symmetry D_5d) cannot be definitely ruled out. The MC and CC bond distances are 2.169(4) and 1.431(2) Å respectively in (C₅H₅)₂Cr, and 2.280(5) and 1.434(3) Å respectively in (C₅H₅)₂V. The CH bonds in (C₅H₅)₂Cr are bent 2.9(1.1)° out of the plane of the carbon atoms towards the metal atom.The molecular structures of the known di-π-cyclopentadienyl compounds of the first row transition elements are compared in the light of what is known about their electronic structures.     

Coordination chemistry of tin: Part III. The crystal structure and thermal behavior of dipotassium dimethyl-tetrafluoro-stannate dihydrate, K2[(CH3)2SnF4]·2H2O

Reaction of (CH₃)₂SnF₂ with two equivalents of KF in aqueous medium leads to the formation of the complex salt K₂[(CH₃)₂SnF₄]·2H₂O (1). Its crystal structure was determined by single-crystal X-ray diffraction. Complex 1 crystallizes in the monoclinic space group C2 (No. 5) with the lattice parameters a=9.265(1), b=7.556(1), c=7.076(1) Å; β=98.21(1)° and Z=2. The structure is characterized by the anion [(CH₃)₂SnF₄]²⁻ in which the tin atom adopts a slightly distorted octahedral coordination, with the methyl groups in trans position. The potassium cations are pentacoordinated from three fluorine atoms and the oxygen atoms of two water molecules in the form of a distorted square pyramid. In addition, the thermal behavior of the compound was studied with the aid of TG/DSC-measurements coupled with MS, revealing that the dehydration of 1 takes place at 75 °C, with an enthalpy of 57.79 kJ mol⁻¹, and that it decomposes without melting in two further endothermic steps to undetermined phases in the system KF-SnF₂-SnF₄ and free carbon (∼0.1%).     

Theoretical study on the structures and properties of the isomers of Nn(CH)8−nH8 (n = 0–7)

With replacement of N atoms by CH groups in the most stable chain isomer of N8H8, 34 possible isomers of N_n(CH)_8−nH₈ (n = 0–7) have been designed and optimized at the B3LYP/6-311++G** level of theory. The natural bond orbital (NBO) and atoms in molecules (AIM) analysis are carried out to study the bonding nature and relative stabilities of these conformers. G3MP2 method is applied to calculate energies and heats of formation. The results indicate that the hyperconjugation effect from lone pairs of nitrogen atoms to germinal C–N bonds is the major factor which caused the change of the C–N bond length. With the more replacement of nitrogen atoms by CH groups, the heats of formation of the isomers of N_n(CH)_8−nH₈ (n = 0–7) decrease gradually, but the energies increase linearly.     

Comparative study on the Al–Al multiple bond in Na2[Arx′AlAlArx′] and H2[Arx′AlAlArx′] (Arx′?=?C6H3-2, 6-(C6H5)2)

The Al–Al multiple bond in Na₂[Arx′AlAlArx′] (Arx′ = C₆H₃-2,6-(C₆H₅)₂) was investigated and compared with H₂[Arx′AlAlArx′] by electron localization function (ELF) method. The roles of sodium, hydrogen atoms, and bulky ligands in these two complexes were also discussed. The calculated results show that Na₂[Arx′AlAlArx′] and H₂[Arx′AlAlArx′] have different structural and electronic features. In Na₂[Arx′AlAlArx′], the Al–Al bond includes a σ bond, a normal π bond and a slipped π bond. In H₂[Arx′AlAlArx′], the direct Al–Al bond was substituted by two 3-center, 2-electron (3c–2e) bridged bonding, which formed by the hydrogen and two aluminum atoms. The bulky ligands play important stabilizing roles in both Na₂[Arx′AlAlArx′] and H₂[Arx′AlAlArx′].