Li2I(OH): Eine Verbindung mit eindimensional unendlich kantenverknüpften [Li4/2(OH)]+-Pyramiden

Li₂I(OH): A Compound with Onedimensional Infinite Edge Sharing [Li_4/2(OH)⁺] Pyramids The pseudobinary system LiOH/LiI was investigated by X-ray methods. Two compounds, Li₂I(OH) and Li₅I(OH)₄ exist. The structure of Li₂I(OH) was solved by single-crystal data. For Li₅I(OH)₄ lattice constants and space group symmetry are given: Li₂I(OH): Pnma, Z = 4, a = 10.339(4) Å, b = 5.567(1) Å, c = 6.643(2) Å, Z(F_o) mit (F_o)² ≧ 3σ(F_o)² = 439, Z (parameter) = 23, R/R_w = 0.030/0.040 Li₅I(OH)₄: Pmmn or P2₁mn(= Pmn2₁), Z = 2, a = 10.42 Å, b = 5.30 Å, c = 5.81 Å Li₂I(OH) crystallizes in a new type of structure. The motif of a distorted hexagonal close-packed arrangement of iodide ions is penetrated by chains of [Li_4/2(OH)⁺].     

A series of oxygen-defect perovskites containing CuII and CuIII: The oxides La3−xLnxBa3 [CuII5−2y CuIII1+2y] O14+y

A series of oxygen-defect perovskites, containing Cu^II and Cu^III, La₃Ba₃ [Cu^II_5?2y Cu^III_1+2y] O_14+y, has been synthesized at 1000°C, for 0.05 ≤ y ≤ 0.43. The substitution of lanthanum for yttrium and lanthanides has been studied. These oxides are tetragonal: $\text{a = a}{}_{\mathrm{<mtext>p</mtext>}}\text{2}{}^{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ and c = 3a_p. The structural study of La₃Ba₃ Cu₆O_14.10 shows that oxygen vacancies are ordered, involving for copper three sorts of coordination: square, pyramidal (4 + 1), and distorted octahedral (4 + 2). The distribution of Cu^III, as well as the lanthanide ions on the different sites, is discussed.     

Ein sauerstoffreiches Neodymcuprat: Hochdrucksynthese und Kristallstruktur von Nd12Cu6O25 („Nd2CuO4,17”︁)

An Oxygen-rich Neodymium Cuprate: High-pressure Synthesis and Crystal Structure of Nd₁₂Cu₆O₂₅ (“Nd₂CuO_4.17”) Single crystals of Nd₁₂Cu₆O₂₅ (“Nd₂CuO_4.17”) could be obtained by reaction of Nd₂O₃ und CuO with KO₂ in a modified Belt-type apparatus at 40 kbar, 1500°C. The compound crystallizes in the monoclinic space group C2/m with a = 17.128(6), b = 3.7288(6), c = 18.364(6) Å, β = 111.22(1)º and Z = 2. The structure refinement converged at R1 = 0.0302 for 1451 reflections with F_o > 4σ(F_o) and R1 = 0.0903, wR2 = 0.0767 for all 2571 data. The structure-determining feature are Cu(1,2)? O octahedral chains, interrupted by Cu(3) atoms in square-planar coordination. Each of this CuO₄ groups is connected to another one, resulting in short copper-copper distances (d_{Cu? Cu} = 3.012 Å). A comparison of the structure of “Nd₂CuO_4.17” with those of La₂CuO₄ and Nd₂CuO₄ makes the structural relations of the former with La₂CuO₄ and, hence, the aristotype K₂NiF₄ evident, in spite of the close stoichiometric similarity between Nd₂CuO₄ and “Nd₂CuO_4.17”.     

Bond stretching and redox behavior in coinage metal complexes of the dichalcogenide dianions [(SPh2P)2CEEC(PPh2S)2]2- (E=S, Se): diradical character of the dinuclear copper(I) complex (E=S)

The metathetical reactions of a) [Li(tmeda)]₂[(S)C(PPh₂S)₂] (Li₂? 3 c ) with CuCl₂ and b) [Li(tmeda)]₂[(SPh₂P)₂CSSC(PPh₂S)₂] (Li₂? 4 c ) with two equivalents of CuCl both afford the binuclear Cu^I complex {Cu₂[(SPh₂P)₂CSSC(PPh₂S)₂]} ( 5 c ). The elongated (C)S? S(C) bond (ca. 2.54 and 2.72 Å) of the dianionic ligand observed in the solid‐state structure of 5 c indicate the presence of diradical character as supported by theoretical analyses. The treatment of [Li(tmeda)]₂[(SPh₂P)₂CSeSeC(PPh₂S)₂] (Li₂? 4 b ) and Li₂? 4 c with AgOSO₂CF₃ produce the analogous Ag^I derivatives, {Ag₂[(SPh₂P)₂CEEC(PPh₂S)₂]} ( 6 b , E=Se; 6 c , E=S), respectively. The diselenide complex 6 b exhibits notably weaker Ag? Se(C) bonds than the corresponding contacts in the Cu^I congeners, and the ³¹P NMR data suggest a possible isomerization in solution. In contrast to the metathesis observed for Cu^I and Ag^I reagents, the reactions of Li₂? 4 b and Li₂? 4 c with Au(CO)Cl involve a redox process in which the dimeric dichalcogenide ligands are reduced to the corresponding monomeric dianions, [(E)C(PPh₂S)₂]^2? ( 3 b , E=Se; 3 c , E=S), and one of the gold centers is oxidized to generate the mixed‐valent Au^I/Au^III complexes, {Au[(E)C(PPh₂S)₂]}₂ ( 7 b , E=Se; 7 c , E=S), with relatively strong aurophilic Au^I???Au^III interactions. The new compounds 5 c , 6 b , c and 7 b , c are characterized in solution by NMR spectroscopy and in the solid state by X‐ray crystallography ( 5 c , 6 b , 7 b and 7 c ) and by Raman spectroscopy ( 5 c and 6 c ). The UV‐visible spectra of coinage metal complexes of the type 5 , 6 and 7 are discussed in the light of results from theoretical analyses using time‐dependent density functional theory.     

Tt‐Tt (Tt = Si,Ge) Dumb‐Bell Structures at Different Valence Electron Concentrations: Ln2MgSi2 (Ln = La,Ce), Yb2Li0.5Ge2, and Yb1.75Mg0.75Si2

The isostructural compounds Yb₂MgSi₂, La_2.05Mg_0.95Si₂, and Ce_2.05Mg_0.95Si₂, as well as Yb₂Li_0.5Ge₂ and Yb_1.75Mg_0.75Si₂, respectively, were synthesized from stoichiometric mixtures of the corresponding elements in sealed Nb‐ ampoules under argon atmosphere. The structures were determined by single crystal X‐ray diffraction: Yb₂MgSi₂ (P4/mbm (No. 127), a = 7.056(1), c = 4.130(1) ų, Z = 2), La_2.05Mg_0.95Si₂ (P4/mbm, a = 7.544(1), c = 4.464(1) ų, Z = 2), and Ce_2.05Mg_0.95Si₂ (P4/mbm, a = 7.425(1), c = 4.370(1) ų, Z = 2), Yb₂Li_0.5Ge₂ (Pnma (No. 62), a = 7.0601(6), b = 14.628(1), c = 7.6160(7) Å, V = 786.5ų, Z = 4), Yb_1.75Mg_0.75Si₂ (Pnma, a = 6.9796(1), b = 14.4009(1), c = 7.5357(1) Å, V = 757.43(2) ų, Z = 4). All compounds contain exclusively Tt‐Tt dumb‐bells (Tt = Si, Ge). The Si‐Si Zintl anions exhibit only very small variations of bond lengths which seem to be more due to cation matrix effects than to effective bond orders.     

Darstellung,Kristallstrukturen und Eigenschaften von Ln4Au2O9 (Ln = Nd,Sm, Eu)

Syntheses, Crystal Structures, and Properties of Ln₄Au₂O₉ (Ln = Nd, Sm, Eu) The compounds Ln₄Au₂O₉ (Ln = Nd, Sm, Eu) have been prepared from amorphous Au₂O₃ · 2–3 H₂O and Ln₂O₃ (Ln = Nd, Sm, Eu) via solid state reaction under elevated oxygen pressure adding KOH as mineralising agent. They are isostructural with La₄Au₂O₉ (Nd₄Au₂O₉: a = 11.9813(3), b = 6.1474(1), c = 11.9641(4); 453 powder intensities, R_p = 3.75%; Sm₄Au₂O₉: a = 11.8689(4), b = 6.0360(1), c = 11.8469(4) Å; 812 unique reflections, R₁ = 2.75%; Eu₄Au₂O₉: a = 11.8241(3), b = 5.9922(1) Å, c = 11.8013(3) Å; 1315 unique reflections, R₁ = 7.83%). The crystal structure of Nd₄Au₂O₉ was refined from powder diffraction data. The structures of Sm₄Au₂O₉ and Eu₄Au₂O₉ were solved and refined from single crystal data. The isolated square planar AuO₄ units are stacked as columns and are linked to each other by LnO₇‐polyhedra. One of the oxygen atoms is exclusively connected to the trivalent lanthanides in tetrahedral geometry. Ln₄Au₂O₉, Bi₂CuO₄, Bi₂AuO₅ and Bi₄Au₂O₉ are closely related, structurally. The lanthanoid aurates decompose between 700 and 800 °C into Ln₂O₃, Au and O₂. The effective magnetic moments 3.64 μ_B (Nd₄Au₂O₉), 1.7 μ_B (Sm₄Au₂O₉) and 3.3 μ_B (Eu₄Au₂O₉) confirm that the lanthanides are trivalent. The UV/VIS absorption spectra can be interpreted at assuming free ions.     

A 2‐D 3d–4f Heterometallic Compound: Hydrothermal Synthesis,Structure and Magnetic Properties

A novel two‐dimensional 3d–4f heterometallic inorganic compound with the formula [Cu^II₃Gd^III(μ₃‐OH)₆(μ₃‐SH)(SO₄)(H₂O)₃] ( 1 ) was synthesized by treating gadolinium nitrate, copper chloride and DTSA under hydrothermal conditions. The structure was determined by X‐ray crystallography. The crystal is of orthorhombic, space group P2₁2₁2₁ with a = 6.63090(1) Å, b = 11.3145(3) Å, c = 15.7869(3) Å, Cu₃GdH₁₃O₁₃S₂, M = 633.09, Z =4, V = 1184.42(4) ų, F(000) = 1200, R₁ = 0.0244 and ωR = 0.0522. The solid‐state dc magnetic susceptibility measurements revealed antiferromagnetic interactions between the paramagnetic metal center ions.     

Anodic synthesis and XPS analysis of La_(1-x)Na_xCu_2O_4

The single phase La1-x NaxCu2O4 crystals were synthesized by an electrochemical method from molten KOH/NaOH/KNO3 at 280-300℃ while La2-yNayCuO4 were prepared by precipitation from the same molten salt. The resulting crystals were characterized by using SEM, XRD, EDX and XPS. XPS analysis revealed that the La3d satellite structures of La1-xNaxCu2O4 were quite different from those of La2-yNayCuO4. These differences have been attributed to the changes in crystal structures, bond lengths and covalent character of the metal-ligand bonds.     

The Reduction of AuF3 in Super Acidic Solution

AuF₃ is reduced in superacidic HF/SbF₅ solutions giving three products. 1. Orange [Au₃F₈·2SbF₅]. It has a layered structure built up by square planar Au^IIF₄ and Au^IIIF₄ units: Crystal structure: space group P2₁/c, a = 9.049(2), b = 8.424(1), c = 9.645(1)Å, β = 115.08(1)°. 2. Black [Au₃F₇·3SbF₅] has a ribbon structure, similarly built up by square planar Au^IIF₄ and Au^IIIF₄ units: Crystal structure: space group Pc, a = 9.991(1), b = 10.728(1), c = 15.222(1)Å, β = 95.304(2)°. 3. Yellow green [(Au(HF)₂] (SbF₆)₂·2HF with square planar Au^IIF₄ units that are formed by two fluorine atoms of the anions and two HF molecules as complex ligands. Crystal structure: Space group P¯, a = 5.482(1), b = 5.848(1), c = 9.309(2)Å, α = 89.522(4), β = 85.635(4), γ = 87.509(4)°.     

Darstellung und Kristallstruktur eines Kalium—Magnesium-Oxocuprat/-vanadats: KMg2Cu2V3O12

Preparation and Crystal Structure of Potassium Magnesium Oxocuprate/-vanadate: KMg₂Cu₂V₃O₁₂ . Single crystals of KMg₂Cu₂V₃O₁₂ were prepared by solid state reactions below the melting point of the reaction mixture (K₂CO₃, MgCO₃, CuO, V₂O₅). It crystallizes with monoclinic symmetry space group C? C2/c, a = 12.1592 Å, b = 12.7204 Å, c = 6.8557 Å, β = 111.73°, Z = 4. The structure type is characterized by VO₄ tetrahedra, twisted CuO₄ square units, MgO₆ octahedra and a special 2 + 4 + 2 coordination around the potassium ion.     

Synthesis and Structure of the New Compound La2O(CN2)2 Possessing an Interchanged Anion Proportion Compared to the Parent La2O2(CN2). Synthese und Kristallstruktur der neuen Verbindung La2O(CN2)2 mit einem vertauschten Anionenverhältnis gegenüber der Bezugsverbindung La2O2(CN2)

La₂O(CN₂)₂ was synthesized from a 1:1:2 molar reaction mixture of LaCl₃, LaOCl, and Li₂(CN₂) at 650 °C. Well developed single crystals were grown from a LiCl‐KCl flux. The crystal structure was refined as monoclinic (space group C2/c, Z = 2, a = 13.530(2) Å, b = 6.250(1) Å, c = 6.1017(9) Å, β = 104.81(2)°) from single crystal X‐ray diffraction data. The La³⁺ and (CN₂)^2— ions in the crystal structure of La₂O(CN₂)₂ can be compared to Fe³⁺ and S₂^2— ions in the cubic pyrite structure, being arranged like in a distorted NaCl type structure with their centers of gravity. In addition, the O^2— ions in La₂O(CN₂)₂ are occupying 1/4 of the tetrahedral voids formed by the arrangement of metal ions.     

Syntheses,Structures, and Properties of New Quaternary Gold-Chalcogenides: K2Au2Ge2S6, K2Au2Sn2Se6, and Cs2Au2SnS4

The new compounds K₂Au₂Ge₂S₆ ( 1 ), K₂Au₂Sn₂Se₆ ( 2 ), and Cs₂Au₂SnS₄ ( 3 ) have been synthesized through direct reaction of the elements with a molten polyalkalithiogermanate(stannate) flux at 650, 550, and 400 °C, respectively. Their crystal structures have been determined by single crystal X-ray diffraction techniques. 1 crystallizes in the monoclinic space group P2₁/n with a = 10.633(2) Å, b = 11.127(2) Å, c = 11.303(2) Å, β = 115,37(3)°, V = 1208,2(3) ų and Z = 4, final R(Rw) = 0.045(0.106). 2 crystallizes in the tetragonal space group P4/mcc with a = 8.251(1) Å, c = 19.961(4) Å, V = 1358,9(4) ų and Z = 4, final R(Rw) = 0.040(0.076). 3 crystallizes in the orthorhombic space group Fddd with a = 6.143(1) Å, b = 14.296(3) Å, c = 24.578(5) Å, V = 2158.4(7) ų and Z = 4, final R(Rw) = 0.039(0.095). The structures of 1 , 2 , and 3 consist of infinite, one-dimensional anionic chains containing X₂Q₆^4– units linked by Au⁺ ions and charge balancing K⁺/Cs⁺ ions situated between the chains. All compounds were investigated with differential thermal analysis, FT-IR, and solid state UV/VIS diffuse reflectance spectroscopy.     

Strukturuntersuchungen an den Oxidnitriden SrTaO2N,CaTaO2N und LaTaON2 mittels Neutronen‐ und Röntgenbeugung

Structural Investigations on the Oxidenitrides SrTaO₂N, CaTaO₂N and LaTaON₂ by Neutron and X‐ray Powder Diffraction The crystal structures of the perovskite related oxidenitrides SrTaO₂N, LaTaON₂ and CaTaO₂N have been determined with special regard to the structures of the respective anionic partial structure. The structure refinements were performed by individual Rietveld analyses of both X‐ray and neutron powder diffractograms and in addition by joint refinements in order to confirm the results. Both refinement methods yield consistent structure solutions. At least the first two compounds have fully ordered anionic sublattices. The crystal structure of SrTaO₂N has been solved in the space group I4/mcm (a = 5.7049(3) Å, c = 8.0499(5) Å, R_p = 0.0706, R_wp = 0.0904, reflections: 70 (neutrons)/36 (X‐ray), R(F²)(n) = 0.147, R(F²)(X) = 0.0952), with an ordered anionic partial structure. LaTaON₂ crystallizes monoclinic (C2/m, a = 8.0922(3) Å, b = 8.0603(2) Å, c = 5.7118(2) Å, β = 134.815(1)°, R_p = 0.0592, R_wp = 0.0766, reflections: 235(n)/113(X), R(F²)(n) = 0.0944, R(F²)(X) = 0.165) and also shows a totally ordered distribution of the anions. In the case of CaTaO₂N (Pnma, a = 5.6239(3) Å, b = 7.8954(4) Å, c = 5.5473(3) Å, R_p = 0.0503, R_wp = 0.0656, reflections 206(n)/110(X), R(F²)(n) = 0.0985, R(F²)(X) = 0.0405) slightly unbalanced displacement parameters (neutron data, ordered O/N distribution model) hint at a partial exchange of oxygen and nitrogen.     

Hydrothermal Synthesis of Brucite Type Copper Hydroxide Squarate [Cu3(OH)2(C4O4)]·4H2O

Herein we report synthesis of a new brucite type copper hydroxide squarate, Cu₃(OH)₂(C₄O₄)₂·4H₂O [P2₁/c, a = 5.6437(4) Å, b = 12.8357(9) Å, c = 9.1507(6) Å, β = 95.892(1)° and Z = 2] by hydrothermal method, and its characterization by single crystal diffraction analysis as well as by IR spectroscopy. The rather wide spread of Cu–O bond lengths, can be primarily rationalised by the Jahn‐Teller effect, and secondarily by the connectivities of the CuO₆ octahedra.     

über Erdalkalimetalloxocuprate,VIII Zur Kenntnis von Sr2CuO2Cl2

On Alkaline Earth Oxocuprates VIII. About Sr₂CuO₂Cl₂ Sr₂CuO₂Cl₂ was prepared and investigated by single crystal X – ray work (space group D–Immm, a = 3.975, c = 15.618 Å). Sr₂CuO₂Cl₂ is isotypic with K₂NiF₄ – compounds and shows an octahedral configuration for Cu²⁺. Cl^? occupies trans-positions of the octahedral Cu²⁺/O^2? polyhedron. A discussion with related compounds (Sr₂CuO₃ and Nd₂CuO₄) explains the observed distribution of O^2? and Cl^?.     

Structural studies in the Li2MoO4MoO3 system: Part 1 the low temperature form of lithium tetramolybdate,LLi2Mo4O13

LLi₂Mo₄o₁₃ crystallizes in the triclinic system with unit-cell dimensions a = 8.578 Å, b = 11.450 Å, c = 8.225 Å, α = 109.24°, β = 96.04°, γ = 95.95° and space group $\text{P}\text{1}\text{, Z = 3}$. The calculated and measured densities are 4.02 g/cm³ and 4.1 g/cm³ respectively. The structure was solved using three-dimensional Patterson and Fourier techniques. Of the 2468 unique reflections collected by counter methods, 1813 with I ? 3σ(I) were used in the least-squares refinement of the model to a conventional R of 0.031 (ωR = 0.038). LLi₂Mo₄O₁₃ is a derivative of the V₆O₁₃ structure with oxygen ions arranged in a face-centred cubic type array with octahedrally coordinated molybdenum and lithium ions ordered into layers.     

Synthesis and Crystal Structure of Na7Cu3O8, Containing a New Type of Oxocuprate(III) Oligoanion

Na₇Cu₃O₈ was prepared through oxidation of a Na₃CuO₂/NaCuO mixture (2:1) in dried oxygen at 450 °C. Single crystals have been grown by annealing of Na₇Cu₃O₈, in the presence of Na₂O₂, at 450 °C for 2000 h in silver crucibles, which were sealed in glass ampoules under dried Ar. According to the X-ray analysis of the crystal structure ( , Z = 1, a = 5.5891(2), b = 6.0945(2), c = 7.8890(3) Å, α = 110.059(2), β = 108.669(2), γ = 90.237(2)°) a new Cu₃O₈^7- oxocuprate anion, consisting of three edge sharing CuO₄ squares, is the prominent structural feature. These anions are aligned parallel to the space diagonal of the unit cell and can be regarded as infinite chains from which every fourth copper atom has been removed. This new representative of an oxocuprate(III) anion gives support to the expectation that the gap between dimeric and infinite edge sharing units of square planar cuprate anions can be closed, in principle.     

Li2Br(NH2): Das erste ternäre Alkalimetallamidhalogenid

Li₂Br(NH₂): The First Ternary Alkali Metal Amide Halide The pseudobinary system LiNH₂/LiBr was investigated by X-ray methods. The crystal structure of the compound Li₂Br(NH₂) was solved by single crystal data: Li₂Br(NH₂): Pnma, Z = 8, a = 12.484(2) Å, b = 7.959(1) Å, c = 6.385(1) Å, Z(F_o) with (F_o)² ≧ 3σ(F_o)² = 348, Z (parameter) = 51, R/R_w = 0.019/0.021 Li₂Br(NH₂) crystallizes in a new type of structure. To one another isolated chains of [Li₂Li_4/2(NH₂)₂²⁺] show the motif of closest rod packing. They are connected via bromide ions in a distorted cubic primitive arrangement.     

Ungewöhnliche Koordinationspolyeder um Sauerstoff in Li4Cl(OH)3

Unusual Coordination Polyhedra around Oxygen in Li₄Cl(OH)₃ The pseudobinary system LiOH/LiCl was investigated by X-ray methods. Two compounds, Li₄Cl(OH)₃ and Li₂Cl(OH), were obtained. The crystal structure of Li₄Cl(OH)₃ solved by single-crystal methods is delt with. For Li₂Cl(OH) powder diffraction data are given: Li₄Cl(OH)₃: P2₁/m, Z = 2, a = 5.4096(8) Å, b = 7.382(2) Å, c = 6.2076(8) Å, β = 94.40(1)°, Z(F_o) with (F_o)² ≧ 3σ(F_o)² = 483, Z (parameter) = 50, R/R_w = 0.022/0.025 Li₂Cl(OH): Pmma, Z = 2, a = 7.680(8) Å, b = 4.001(7) Å, c = 3.899(6) Å The hydroxide rich compound crystallizes in a new type of structure which contains puckered layers [Li₄(OH)₃⁺] connected via chloride ions.     

Crystal structures of CrH2P3O10 and InH2P3O10

The crystal structures of chromium and indium dihydrogen triphosphates, CrH₂P₃O₁₀ and InH₂P₃O₁₀, in modification II are refined by the Rietveld method using X-ray powder diffraction data. The compounds crystallize in the monoclinic crystal system, space group P21/n. Z = 4, a = 7.3225(4)Å, b = 8.6835(6)Å, c = 11.6599(7) Å, and b = 102.388(3)° for CrH₂P₃O₁₀, and a = 7.5332(1)Å, b = 9.0841(1)Å, c = 11.8600(1) Å, and b = 103.9596(7)° for InH₂P₃O₁₀. The structures are refined in the isotropic approximation (pseudo-Voigt profile function): R_p = 4.8%, R_wp = 6.9%, R_Bragg = 7.5%, R_F = 9.9% for CrH₂P₃O₁₀; R_p = 6.3%, R_wp = 8.3%, R_Bragg = 6.2%, R_F = 4.1% for InH₂P₃O₁₀. The crystal structures of compounds in the isostructural series M^IIIH₂P₃O₁₀-II, where M^III = Al, Ga, Cr, V, Fe, and In, are examined and compared.