Structure and thermal properties of [Ir(NH3)5Cl]x[Rh(NH3)5Cl]1?xMO4 (x = 0.5, 1; M = Mo, W)

Complex salts [Ir(NH₃)₅Cl]x[Rh(NH₃)₅Cl]_1−x MO₄ (x = 0.5, 1; M = Mo, W) are synthesized and their thermal properties are studied. The crystal structures are determined for [Ir(NH₃)₅Cl]WO₄ and [Ir(NH₃)₅Cl]MoO₄. In the structures, the ions are linked by N-H...O hydrogen bonds, the shortest ones being 2.868(2)–3.422(2) ?. and 2.860(4)–3.434(3) ?. respectively. The thermal properties of the complex salts are studied in the hydrogen atmosphere and in hydrogen-helium mixtures. It is demonstrated that the final products are the mixtures of nanocrystalline powders of Ir and binary or ternary solid solutions with the hcp lattice.     

Crystal structure of Sm(Phen)(i-Bu2PS2)3·MeCN and photoluminescence properties of SmL(i-Bu2PS2)3 (L = Phen, 2,2′-bipy)

It is revealed that at 300 K Sm(Phen)(i-Bu₂PS₂)₃ (I) and Sm(2,2′-Bipy)(i-Bu₂PS₂)₃ (II) complexes have photoluminescence properties typical of the Sm³⁺ ion. In the spectra, three bands are observed with 7n_max = 564 nm, 600 nm, and 645 nm. Single crystals of Sm(Phen)(i-Bu₂PS₂)₃·MeCN (III) are grown, and the structure of the compound is determined based on the X-ray diffraction data (X8 Apex diffractometer, MoK6h radiation, 7685 F _hkl, R = 0.0258). Crystals of III are triclinic, unit cell parameters are a = 11.0554(3) ?, b = 15.0446(3)?, c= 15.4849(4)?; 6h = 89.218(1)°, β = 75.555(1)°, γ = 73.484(1)°, V= 2386.6(1)?³, Z=2, ρ_calc = 1.391 g/cm³, P1 space group. The structure of III is formed from the molecules of mononuclear complex I and MeCN molecules. A coordination polyhedron of the Sm atom is an N₂S₆ tetragonal antiprism. It is shown that the structure of III includes dimeric assemblies of the molecules of complex I.     

Synthesis and thermolysis of substitutional solid solutions (Cu1?yMy)2(OH)PO4·xH2O (x = 0.1?0.2; M = Zn, Co, Ni)

Substitutional solid solutions (Cu_1−y Zn _y )₂(OH)PO₄·xH₂O (0 ≤ y ⩽ 0.26, x = 0.1−0.2), (Cu_1−y Co _y )₂(OH)PO₄·xH₂O (0 ≤ y ≤ 0.10, x = 0.1−0.2), and (Cu_1−y Ni _y )₂(OH)PO₄·xH₂O (0 ≤ y ≤ 0.08, x = 0.1−0.2) were synthesized. The unit cell parameters of the resulting phosphates were determined, and their IR absorption spectra were measured. The reactants were H3PO4 and mixtures of hydrous carbonates of the appropriate metals. Thermolysis of the solid solutions was examined with (Cu_1−y Co _y )₂(OH)PO₄·xH₂O (0 ≤ y ≤ 0.10, x = 0.1−0.2) as an example.     

Effects of combined substitution of Dy and Mo or Si on the crystal structures and magnetic properties of Nd1?yDyyFe11?xTiMx (M = Mo, Si) compounds

A series of Nd_1−y Dy _y Fe_11−x TiM_x (M = Mo, Si) alloys have been prepared by arc melting and studied by X-ray diffraction and neutron diffraction. All samples are found to crystallize in the ThMn₁₂-type structure. The lattice parameters a and c and unit cell volume V of Nd_0.5Dy_0.5Fe_11−x TiMo _x alloys increase linearly with increasing content of Mo (x), while the lattice parameters a and c and unit cell volume V of Nd_0.5Dy_0.5Fe_11−x TiSi _x alloys decrease linearly with increasing content of Si(x). In Nd _y Dy_1−y Fe_11−x TiM _x (M = Mo, Si) compounds, Ti and Mo atoms preferentially occupy the 8i sites and Si atoms preferentially occupy the 8j and 8f sites. Magnetic measurements show that the substitution of Fe by either Mo or Si leads to a decrease in the Curie temperature. Supported by the National Natural Science Foundation of China (Grant No. 20775088) and the Foundation of State Key Laboratory of Environmental Chemistry and Ecotoxicology, Research Center for Eco-Environmental Sciences, Chinese Academy of Sciences (Grant No. KF2008-06)     

New supramolecular adducts of chloroaquacomplexes [M3(μ3-S)S3?xSexCly(H2O)9?y](4?y)+ (M = Mo, W) with cucurbit[6]uril

New supramolecular adducts of cucurbit[6]uril with triangular cluster chloroaquacomplexes of Mo and W with mixed sulfido-selenido bridging ligands, {[W₃S₃Se(H₂O)₇Cl₂]₂(C₃₆H₃₆N₂₄O₁₂)}Cl₂·15H₂O (1), {[W₃S_1.5Se_2.5Cl_1.5(H₂O)_7.5]₂(C₃₆H₃₆N₂₄O₁₂)}Cl₅·18.5H₂O (2), and {[Mo₃SSe₃(H₂O)_7.5Cl_1.5]₂× (C₃₆H₃₆N₂₄O₁₂)}C_l5·11H₂O (3) are obtained treating the mixture of products in Mo-S-Se-Br and W-S-Se-Br systems, isolated, and structurally characterized. In all compounds, the supramolecular structure is based on hydrogen bonded associates of cucurbit[6]uril molecule with two cluster cations.     

Synthesis and study of the properties of K2Y1 ? x ? yEuxTby(MoO4)(PO4) and K2Y1 ? x ? yEuxTby(MoO4)(PO4)1?δ(VO4)δ solid solutions

Al synthesized samples are isostructural and crystallize in the orthorhombic symmetry system, space group Ibca. Particles of the final product of ∼200 nm in size have been obtained. The introduction of the vanadate anion into the matrix composition leads to the lowering of the symmetry of the Eu³⁺ environment and to the rise of the defect luminescence at 450–550 nm because of the unit cell distortion. The luminescence of defects in terbium-europium-containing samples is determined by the sample surface area, which decreases on annealing. The τ, W ₀ and γ parameters of the luminescence kinetics of the samples have been determined.     

Isomerism of [FeMM′(μ3-Q)(CO)7CpCp′] heterometallic clusters (Q = Se, Te; M, M′ = Mo, W; Cp = η5-C5H5; Cp′ = Cp, η5-C5(CH3)5) in solids

The crystal structures of three cluster compounds: [(µ-H)Fe₂Mo(µ₃-Te)(CO)₈Cp*], [FeMo₂(µ₃-Te)(CO)_7x Cp*₂], and [FeMoW(µ₃-Te)(CO)₇CpCp*], where Cp = ⁵-C₅H₅, Cp* = ⁵-C₅ (CH₃)₅, have been investigated. In the cluster with a tetrahedral {FeMo₂Te} core, one can observe positional isomerism of the carbonyl and cyclopentadienyl ligands with respect to the plane through the Fe and Te atoms and the center of the Mo₂bond, resulting in two mirror isomers in the racemic crystal. In the cluster with the {FeMoWTe} core, additional chirality causes the formation of four diastereoisomers. Earlier, the structure of the [FeMoW(µ₃-Se)(CO)₇Cp] cluster with Mo and W atoms coordinated to identical Cp-ligands has been structurally defined. In this crystal, statistical disordering of Mo and W over the metal positions is observed. In the [FeMo(Cp*)W(Cp)(µ₃-Te)(CO)₇] cluster studied here, the Mo and W atoms are coordinated to different cyclopentadienyl ligands. Due to this, two of four diastereoisomers were isolated as ordered racemic crystals; the other two are nonexistent for steric reasons.Original Russian Text Copyright © 2004 by A. V. Virovets, S. N. Konchenko, P. S. Yuferov, and D. FenskeTranslated from Zhurnal Strukturnoi Khimii, Vol. 45, No. 3, pp. 522–527, May–June 2004.     

Coordination compounds of electron-deficient boron cluster anions BnH n2? (n = 6, 10, 12)

This survey concerns the coordination ability of B _n H _n ²⁻ (n = 6, 10, 12) boron cluster anions and their derivatives in complex formation. Boron cluster anions form four types of compounds: salts of organic cations and alkali-metal cations, including Cat₂B _n H _n , where specific interactions can be observed between a cation Cat and a boron cluster anion; salts of protonated anions CatB₆H₇ and CatB₁₀H₁₁, analogues of Cat[MB _n H _n ] complexes, where an extra hydrogen atom appears bound with the BBB face of a boron polyhedron and performs as a hard acceptor; metal complexes with outer-sphere boron cluster anions where specific ligand-ligand interactions may be observed between a boron cluster anion and an inner-sphere ligand; and true metal complexes with boron cluster anions that enter the inner coordination sphere. The last case characterizes closo-hydroborate anions as polydentate ligands whose denticity can vary widely under the effect of substituents or other ligands in the complex.     

A study of YBa2(Cu1?xMex)3O6 + δ (Me = Al, Co, Fe) electrophysical and electrochemical properties

The structure, thermal expansion coefficient, and electroconductivity of YBa₂(Cu_1−x Al _x )₃O_6+δ (x = 0.0–0.9) were studied at 20 to 900°C in air. The most conducting compositions of YBa₂(Cu_1−x Me _x )₃O_6+δ (Me = Al, Co, Fe) were determined. The electrochemical activity of electrodes with the most conducting compositions of YBa₂(Cu_1−x Me _x )₃O_6+δ (Me = Al, Co, Fe) was studied in a wide polarization range in the contact with 0.9ZrO₂ + 0.1Y₂O₃ solid electrolyte in air at the temperatures of 700 to 900°C. Original Russian Text ? V.K. Gil’derman, I.D. Remez, 2009, published in Elektrokhimiya, 2009, Vol. 45, No. 5, pp. 612–615. Published by report at IX Conference “Fundamental Problems of Solid State Ionics”, Chernogolovka, 2008.     

Crystal structures of mixed-ligand complexes [CoPhen{(i-C4H9)2PS2}2], [Co(2,2′-Bipy){(i-C4H9)2PS2}2] and the development of dimer assemblies in them

X-ray diffraction data have been used to determine crystal structures of coordination compounds [CoPhen{ (i-C₄H₉)₂PS₂}₂] (I) and [Co(2,2′-Bipy){ (i-C₄H₉)₂PS₂}₂] (II) (X8-APEX diffractometer, MoK _α∔ -radiation, 3083 F _hkl , R = 0.0647 for I and 5381 F _hkl , R = 0.0597 for II). I is triclinic, a = 11.244(1) Å, b = 14.892(2) Å, c = 21.419(4) Å, α = 71.867(4)°, β = 81.553(4)°, γ = 76.777(4)°, V = 3306,9(8) ų; Z = 4, ρ_calc = 1.321 g/cm³, space group ; II is monoclinic, a = 14.693(2) Å; b = 20.868(3) Å, c = 11.417(1) Å; β = 106.46(5)°; V = 3357.1(7) ų, Z = 4, ρ_calc = 1.254 g/cm³, space group P2₁/c. The structures are built from discrete mononuclear molecules. Coordination polyhedra of Co atoms are distorted octahedra formed by four S atoms of two bi-dentate chelating ligands (i-C₄H₉)₂PS ₂ ⁻ and two N atoms of two bi-dentate chelating Phen or 2,2′-Bipy molecules. The interaction of the molecules in the structures of I and II has been analyzed. It has been found that the molecules of I and II form dimer ensembles owing to π-π-interactions of Phen or 2,2′-Bipy. Original Russian Text Copyright ? 2005 by R. F. Klevtzova, L. A. Glinskaya, T. E. Kokina, and S. V. Larionov __________ Translated from Zhurnal Strukturnoi Khimii, Vol. 46, No. 4, pp.705–714, July–August, 2005.     

Exchange coupling in alkoxy-polyoxovanadates [VIVnVV6?nO7(OR)12]4?n (n = 4, 3, 2)

The molecular structure and magnetic properties of alkoxy-polyoxovanadates [V^IV _n V^V _6−n O₇(OR)₁₂]⁴⁻ⁿ (n = 4, 3, 2) were studied within the framework of the DFT approach. The equilibrium geometric configurations of all complexes studied in this work are characterized by a distorted octahedral hexavanadate core; the unpaired d-electrons are localized on the metal centers (V^IV). The localized spin density distribution is also retained in the low-temperature crystal structures of the compounds whose magnetic properties are described by the Heisenberg-Dirac-van Vleck exchange spin Hamiltonian. The exchange parameters calculated using the broken symmetry formalism suggest predominance of ferromagnetic coupling between vanadium(IV) ions in the μ-OR bridged dimeric units {V^IVO(OR)V^IV} and in the diagonal pairs {V^IVOV^IV} (n = 4). The results obtained indicate that the magnitude and sign of the exchange parameters in the isostructural dimeric units within the hexavanadate core depend on the total number of unpaired electrons in the system.     

Synthesis, structure, and properties of M[VO2(XO4)(H2O)2] · H2O (X = S, M = K, Rb, NH4, Tl; X = Se, M = K, Rb, NH4)

Keeping of MVO(XO₄)₂ under saturated vapor pressure at room temperature resulted in the synthesis of a number of isostructural complexes M[VO₂(XO₄)(H₂O)₂] · H₂O, where X = S, M = K, Rb, NH₄, Tl and X = Se, M = K, Rb, NH₄. The conclusion about the isostructural nature of the synthesized sulfate and selenate compounds was based on X-ray diffraction and vibrational spectroscopy data. Characteristic features of the thermal decomposition of M[VO₂(XO₄)(H₂O)₂] · H₂O on heating in air were identified. It was shown that K[VO₂(SeO₄)(H₂O)₂] · H₂O tends to undergo spontaneous dehydration under ambient conditions to give the monohydrate K[VO₂(SeO₄)(H₂O)].     

Synthesis and X-ray diffraction study of complex oxides of the Zn2 ? x(ZraSnb)1 ? xFe2xO4 composition

A multicomponent system of complex refractory oxides of the composition Zn_{2 − x} (Zr _a Sn _b )_{1 − x} Fe_2x O₄ (a + b = 1; a: b = 1: 5, 1: 4, 1: 3, 1: 2, 1: 1, 2: 1, 3: 1, 4: 1; x = 0−1.0; Δx = 0.05) was studied by X-ray diffraction. The samples were prepared from oxides of appropriate metals by low-temperature plasma synthesis (hydrogen-oxygen flame). Two phases with wide homogeneity ranges were identified: α phase crystallized in the crystal system of inverse cubic spinel and β phase with the structure of tetragonal spinel. The phase boundaries were found. Structural data are presented for about 100 solid solutions.     

Isomerism of metal complexes with the boron cluster anions B10H 102? and B12H 122?

A new type of inner-sphere isomerism in coordination chemistry observed in metal complexes with boron cluster anions B _n H _n ²⁻ (n = 10, 12) is discussed. Specific structure of the closo-borohydride anions gives rise to edge and facial isomers, among which mirror isomers have been found. Examples of edge and facial isomers of metal complexes with the B₁₀H₁₀²⁻ and B₁₂H₁₂²⁻, anions obtained experimentally and studied by X-ray diffraction are considered. Analysis of their structure revealed a new type of isomerism, which was called “positional.”     

Li+/H+ ion exchange in Li3 ? 2xNbxM2 ? x(PO4)3 (M = In, Fe) materials with a NASICON structure

H_{3 − 2x} Nb _x M_{2 − x} (PO₄)₃ (M = In, Fe) acid phosphates have been obtained by ion exchange from their lithium forms and X-ray powder diffraction, impedance measurements, and ⁷Li and ¹H NMR spectroscopy. The parameters of the hexagonal unit cell of the proton-exchanged forms differ only slightly from those of the initial lithium compounds. According to ¹H NMR data, the proton in the acid phosphates is not hydrated. The conductivity of the acid phosphates at high temperatures depends weakly on their composition and is ∼1.7 × 10⁻⁷ S cm⁻¹ at 620 K. The activation energy of conduction is 30–33 kJ/mol (430–770 K).     

Syntheses, structures and properties of five chiral quaternary sulfides, AlxLn3(SiyAl1?y)S7 (Ln = Y, Gd, Dy) and In0.33Sm3SiS7

Five new quaternary isostructural rare-earth sulfides, Al_0.57Gd₃(Si_0.27Al_0.73)S₇ (1), Al_0.55Dy₃(Si_0.34Al_0.66)S₇ (2), Al_0.50Y₃(Si_0.50Al_0.50)S₇ (3), Al_0.44Gd₃(Si_0.70Al_0.30)S₇ (4) and In_0.33Sm₃SiS₇ (5), have been synthesized by facile solid-state reactions. They crystallize in the 3-D ALn₃EQ₇ structure type in the hexagonal chiral space group P6₃. The structures feature a 3-D host framework constructed by Ln-S bicapped trigonal prisms, in which the octahedral and tetrahedral interspaces are occupied by A and E atoms, respectively. The investigation of optical and magnetic properties of 4 indicates that it is a semiconductor and behaves antiferromagnetic-like interaction.     

The conditions of formation and physicochemical properties of Nd1 ? xBaxMn1 ? yFeyO3 phases

The homogeneity regions of Nd_{1 − x} Ba _x MnO₃ (0.0 ≤ x ≤ 0.25) and NdMn_{1 − y} Fe _y O₃ (0.0 ≤ y ≤ 1.0) orthorhombic solid solutions in air at 1373 K were determined. The region of the existence of Nd_{1 − x} Ba _x Mn_{1 − y} Fe _y O₃ orthorhombic solid solutions in air at 1373 K was studied. A fragment of the phase diagram of the NdMnO₃-BaMnO₃-BaFeO_2.5-NdFeO₃ quasi-quaternary complex oxide system in air at 1373 K was suggested. The mechanothermal properties of Nd_0.75Ba_0.25MnO₃, Nd_0.8Ba_0.2Mn_0.9Fe_0.1O₃, Nd_0.8Ba_0.2Mn_0.7Fe_0.3O₃, and Nd_0.8Ba_0.2Mn_0.5Fe_0.5O₃ doped neodymium manganates were studied.     

Structural and electric properties of the Ce0.8(Sm1 ? xCax)0.2O2 ? δ system (x = 0.0–1.0)

CeO₂-based solid solutions with a fluorite structure are promising materials as electrolytes of medium-temperature electrochemical devices. This work presents the results of systematic studies of structural and electric properties and oxygen nonstoichiometry of the Ce_0.8(Sm_{1 − x} Ca _x )_0.2O_{2 − δ} system in a wide range of concentrations of 0 < x < 1 performed in order to establish the causes affecting the system conductivity and its behavior in a reducing medium. It is found that a single-phase solid solution of the fluorite type is formed in the whole concentration range. Parameters of its lattice cells decrease linearly at an increase in the concentration of Ca²⁺. Conductivity in air grows when calcium is added due to a decrease in the grain boundary resistance. The maximum conductivity in air was obtained for the composition of Ce_0.8(Sm_0.8Ca_0.2)_0.2O_{2 − δ} and is 13.71 × 10⁻³ S/cm at 873 K. Studies of the dependence of conductivity of the partial pressure of oxygen showed that electron conductivity is observed at a higher oxygen partial pressure at an increase in the temperature and calcium concentration. The critical partial pressure of oxygen ( p_O2 ^* )\left( {p_{O_2 }^* } \right) for the compositions of Ce_0.8(Sm_{1 − x} Ca _x )_0.2O_{2 − δ} with x = 0; 0.2, and 0.5 is 1.83 × 10⁻¹⁶, 1.73 × 10⁻¹³, and 3.63 × 10⁻¹³ atm at 1173 K, respectively, and 2.76 × 10⁻²¹, 5.05 × 10⁻¹⁸, and 1.31 × 10⁻¹⁸ atm at 1023 K.     

Structure and thermal properties of [RhPy4Cl2]X complex salts (X = Cl?, ReO 4? , ClO 4? )

[RhPy₄Cl₂]Cl·4H₂O (I), [RhPy₄Cl₂]ReO₄ (II), [RhPy₄Cl₂]ClO₄ (III), and [RhPy₄Cl₂]ReO₄·2H₂O complex salts were synthesized. The crystal structure of compounds II (P4/ncc, a = 25.5655(3) ?, c = 14.3521(4) ?), III (P2₁/n, a = 13.5308(3) ?, b = 15.1044(5) ?, c = 23.3457(8) ?, β = 93.327°), and dyhydrate of II (Pbcm, a = 10.6199(9) ?, b = 10.4964(9) ?, c = 22.9834(16)?) was determined by X-ray diffraction analysis. The thermal transformations of the complexes were studied by differential thermal analysis. The substances were characterized by IR spectroscopy, XRPA, and element analysis Original Russian Text Copyright ? 2009 by D. B. Vasilchenko, I. A. Baidina, E. Yu. Filatov, and S. V. Korenev __________ Translated from Zhurnal Strukturnoi Khimii, Vol. 50, No. 2, pp. 349–356, March–April, 2009.     

Complex salts trans-[Rh(β-Pic)4Cl2]X (X = Cl?, ReO 4? , and ClO 4? ): Synthesis, crystal structures, and thermal properties

Three novel complex salts containing the cation trans-[Rh(β-Pic)₄Cl₂]⁺ with the anions Cl⁻ (I), ReO₄⁻ (II), and ClO₄⁻ (III) were obtained and characterized by elemental analysis, X-ray diffraction, NMR spectroscopy, and IR spectroscopy. The complex trans-[Rh(β-Pic)₄Cl₂]ReO₄ crystallizes from DMF as a solvate in which solvent molecules fill the channels formed by the cations and anions. The thermal properties of complexes I, II, and II · DMF were examined by DTA. Final and some intermediate products of the thermolysis were isolated and characterized by physicochemical methods.