Zur Darstellung und Struktur von LaTa3O9 Röntgenographische und elektronenmikroskopische Untersuchungen

Preparation and Structure of LaTa₃O₉. X-Ray and Electronmicroscopic Investigations In the system La₂O₃/Ta₂O₅ a new ternary compound LaTa₃O₉ could be prepared by chemical transport in a temperature gradient T₂ → T₁ (1100 → 1040°C; Cl₂ was added). LaTa₃O₉ is orthorhombic, space group Pnma–D with the lattice constants a = 6.59₅, b = 7.66₄, and c = 12.48₁ Å. In the structure ribbons of pentagonal TaO₇-bipyramids are recognizable parallel to the a-direction. These ribbons are connected with each other in the (010) plane by TaO₆-octahedra. The tunnels formed in this way are occupied by La atoms. High resolution transmission electron microscopy images of the structure were made along the [010] direction. They were interpreted by using images calculated on the basis of the multi-slice method.     

Zur Darstellung und Struktur neuer Modifikationen von CeTa3O9

Preparation and Structure of New CeTa₃O₉ Modifications The modifications M? , O? and P? CeTa₃O₉ could be prepared by chemical transport reactions (T₂ → T₁; T₂ = 1100°C; T₁ = 1000°C) with chlorine as transport agent. M? CeTa₃O₉ crystallizes in the monoclinic space group C 2/m with a = 12.415(1) Å, b = 7.6317(8) Å, c = 6.5976(8) Å, β = 93.31(1)°; Z = 4; R = 4.88%, R_w = 3.67%. The structure consists of two types of Ta? O-polyhedra. Especially remarkable are chains of edge sharing pentagonal TaO₇-bipyramids which are connected by TaO₆-octahedra at opposite sides. Tunnels running along [010] are created by the framework of Ta? O-polyhedra and are filled with Ce in levels of y = 1/2 and y = 0. O? CeTa₃O₉ crystallizes orthorhombically with a = 6.5429(7) Å, b = 7.6491(7) Å, c = 12.583(1) Å and is isostructural to O? LaTa₃O₉ (space group: Pnma). O? CeTa₃O₉ contains the same characteristic structural units namely pentagonal TaO₇-bipyramides and TaO₆-octahedra. The difference between O? and M? CeTa₃O₉ is based on the orientation of the tunnels: in the orthorhombic modification they are arranged zigzag-like, in the latter parallel. Both modifications of CeTa₃O₉ can be irreversibly converted into the well-known perovskite-related P? CeTa₃O₉ structure with a lower density by heating in air to 1200°C.     

Zur Darstellung und Struktur von LaNb5O14

Preparation and Structure of LaNb₅O₁₄ Single crystals of LaNb₅O₁₄ could be prepared by chemical transport reactions (T₂ → T₁; T₂ = 1050°C; T₁ = 950°C) using chlorine as transport agent. LaNb₅O₁₄ crystallizes in the orthorhombic space group Pbem with cell dimensions a = 3.8749(2) Å; b = 12.4407(6) Å and c = 20.2051(9) Å; Z = 4; R = 6.28%, R_w = 3.74%. The structure consists of two types of Nb? O-polyhedra. Especially remarkable are chains of edge-sharing pentagonal NbO₇-bipyramids, which are interconnected by corner-sharing NbO₆-octahedra. Tunnels running in a-direction are created by this framework of NbO₆- and NbO₇-polyhedra. Lanthanum atoms are located in these tunnels at levels inbetween the niobium atoms. The relationship to O? LaTa₃O₉ and M? CeTa₃O₉ type structures will be discussed.     

Zum chemischen Transport von Verbindungen des Typs LnTa7O19 (Ln = La?Nd) mit einer Bemerkung zur Strukturverfeinerung von NdTa7O19

Chemical Transport Reactions of Compounds LnTa₇O₁₉ (Ln = La? Nd) and Structure Refinement of NdTa₇O₁₉ Crystals of compounds LnTa₇O₁₉ (Ln ? Na? Nd) could be obtained by chemical transport reactions (T₂ → T₁; T₂ = 1100°C, T₁ = 1000°C) using chlorine (p(Cl₂; 298 K) = 1 atm) as transport agent. An increase of transport rate and an improvement of crystal growth was observed if small amounts of vanadium metal were added. Solid state reactions with mixtures of Ln₂O₃/Ta₂O₅ (1:7) in air (T ≈ 1400–1500°C), however, were not succesful because the resulting samples contained LnTa₇O₁₉ with other ternary phases as by-products. NdTa₇O₁₉ crystallizes in the well-known LaTa₇O₁₉-type structure with cell dimensions of a = 6.2229(3) Å, c = 19.939(2) Å and Z = 2. The crystal structure was refined in space groups P6 c2 (R = 3.35%, R_W = 2.67%) and P6₃/mcm (R = 4.75%, R_W = 3.88%). Taking aspects of structural chemistry, x-ray results and MAPLE calculations into account, however, the spacegroup P6 c2 should be preferred.     

Zur Darstellung und Struktur von M1?LnTa3O9 (Ln = Pr,Nd) Röntgenographische und elektronenmikroskopische Untersuchungen

Preparation and Structure of M1? LnTa₃O₉ (Ln = Pr, Nd), X-Ray and Electronmicroscopical Investigations New ternary compounds M1? LnTa₃O₉ (Ln = Pr, Nd) could be prepared by chemical transport reaction in a temperature gradient T₂ → T₁ (T₂ = 1100°C; T₁ = 1000°C; CI₂ as transport agent). M1 NdTa₃O₉ crystallizes in the monoclinic space group P 2₁/m with a = 5.3840(9) Å, b = 7.550(1) Å, c = 8.1911(9) Å and β = 92.46(1)°. The structure was refined to give R = 6.29% and R_w = 6.20%. It is built of double and single chains of corner-sharing TaO₆ octahedra extended along the b-axis. Tunnels running along [010] are created by the framework of TaO₆ octahedra. Ln (Ln = Pr, Nd) is located in these tunnels to levels of y = 1/4 and 3/4. A structure refinement for isostructural M1? PrTa₃O₉ led to a = 5.4051(7) Å, b = 7.5680(2) Å, c = 8.1964(9) Å, β = 92.38(2)° and R = 7.72%, R_w = 7.57%. By grinding in an agate mortar M1? LnTa₃O₉ transforms into M2? LnTa₃O₉, a new modification with a higher density. High resolution transmission electron microscopy images of the M1? PrTa₃O₉ structure were made along the [010] direction. They could be interpreted by comparing them with images calculated on the basis of the multi-slice method.     

Beiträge zum thermischen Verhalten und zur Kristallchemie wasserfreier Phosphate. XI. Darstellung und Kristallstruktur einer triklinen Modifikation von GeP2O7

Contributions on the Thermal Behaviour and Crystal Chemistry of Anhydrous Phosphates. XI. Synthesis and Crystal Structure of a Triclinic Modification of GeP₂O₇ A new triclinic modification of GeP₂O₇ can be obtained by hydrolysis of GeCl₄ in conc. H₃PO₄ as a microcrystalline powder. Chemical transport experiments (950 → 850°C, transport agent: Cl₂; p = 0.1 atm (298 K)) lead to the formation of small prisms (edge lengths up to 0.7 mm) of high refractive index at the lower temperature zone. The crystal structure determination [Spcgrp.: P1 ; Z = 2; a = 7.730(1) Å; b = 6.724(1) Å; c = 4.6543(8) Å; α = 105.39(1)°; β = 92.81(1)°; γ = 91.49(1)°; 1 358 independent I₀; 94 parameters; conventional residual R1 = 3.1%] shows CN = 6 for Ge (regular octahedra: d?_{Ge1? O} = 1.86 Å; d?_{Ge2? O} = 1.85 Å) and P₂O₇-groups (d?_{P1? O} = 1.53 Å; d?_{P2? O} = 1.53 Å) with ∠ (P? O? P) = 126.5°. All O exhibit twofold coordination which is achieved either by two P or by one Ge- and one P. This modification of GeP₂O₇ bears a close relationship to the crystal structure of PtP₂O₇ and to the [MoP₂O₇]-host lattice of Na_0.3MoP₂O₇. Remarkable differences to the well known cubic structures of many other metal(IV)-diphosphates occur.     

Zur Darstellung und Struktur neuer Niobate LnNb7O19 (Ln = La,Ce)

Preparation and Structure of LnNb₇O₁₉ (Ln = La, Ce) Two new ternary compounds, LaNb₇O₁₉ and CeNb₇O₁₉, could be prepared and characterized. At temperatures about 900°C already decomposition of both compounds will be initiated, but at lower temperatures (800°C) no reaction between the binary components occured. Single crystals could be obtained by chemical transport reactions (T₂ → T₁; T₂ = 800°C; T₁ = 780°C). Chlorine for mineralization or as transport agent is absolutely indispensable for preparation. Single crystal investigations on LaNb₇O₁₉ (R = 4.4%; R_w = 4.19%) result in the trigonal space group P3. The cell dimensions are a = 6.2531(2) A; c = 20.0685(10) Å; Z = 2. The structure can be described as to be build up by layers of 8-coordinated La and 6-coordinated Nb, alternating with layers of edge-sharing pentagonal NbO₇-bipyramids. Corresponding to the unusual sequence of layers the structure of LnNb₇O₁₉ (Ln = La,Ce) is the first example of a trigonal member of a family of structures, which has been described in detail by Jahnberg. The most examples are represented by tantalates, but only a few niobates related to these structures are known.     

Darstellung und Struktur von U2Ta6O19, einer neuen Verbindung mit „Jahnberg‐Struktur”︁, sowie Anmerkungen zu den ersten Oxidchloriden in den Systemen Th/Nb/O/Cl und Th/Zr(Hf)/Nb/O/Cl

Synthesis and Crystal Structure of U₂Ta₆O₁₉, a New Compound with “Jahnberg‐Structure” and a Note to the First Oxide Chlorides in the Systems Th/Nb/O/Cl and Th/Zr(Hf)/Nb/O/Cl Black crystals of U₂Ta₆O₁₉ with hexagonal shape were obtained (at T₁) by chemical transport using HCl (p (HCl, 298 K) = 1 atm; silica tube) as transport agent in a temperature gradient (T₂ → T₁; 1000 °C → 950 °C) and using a mixture of UO₂, Ta₂O₅, and HfO₂ (or ZrO₂) (1 : 2 : 2) as starting materials (at T₂). For the structure determination the best result was achieved in space group P6₃/mcm (No. 193, a = 6.26(2) Å, c = 19.86(6) Å). U₂Ta₆O₁₉ is isotypical to Th₂Ta₆O₁₉. In the crystal structure each uranium atom is surrounded by oxygen atoms like a bi‐capped trigonal antiprism and tantalum atoms like a pentagonal bipyramid (CN = 7). Like the “Jahnberg Structures” both coordination polyhedra arrange themselves in separate layers (U–O‐polyhedra, in o‐, Ta–O‐polyhedra in p‐layers) so that in the direction of the c‐axis the sequence of layers is p‐p‐o. Using chemical transport it was possible to prepare the compounds Th₁₂Nb₁₆O₆₃Cl₂ and Th₈M₄Nb₁₆O₆₃Cl₂ (M = Zr, Hf), which are the first quaternary and quinquinary examples in these systems. They crystallize isotypically.     

Einkristallstrukturaufklärung und elektronenmikroskopische Untersuchungen an einem neuen Uranniobat: γ-UNbO5

X-Ray Single Crystal and Electron Microscopic Investigations on a New Uranium Niobate: γ-UNbO₅ Black cuboid formed crystals of γ-UNbO₅ were obtained (at T₁) by chemical transport in a temperature gradient (T₂ → T₁; 1000 °C → 980 °C) using UNb₂O₇ as starting material (at T₂) and a combination of NbCl₅ and Cl₂ as transport agent. They were examined by X-rays and electron microscopy. The new modification of γ-UNbO₅ crystallizes orthorhombically (space group Pmma) with a = 7.492(3) Å, b = 4.124(4) Å and c = 6.434(4) Å. The compound is isostructural to UVO₅ and UMoO₅. The crystal structure shows parallel layers formed by edge sharing UO₇ and NbO₆ polyhedra. Polyhedra of neighbouring layers (distance = b) are mutually corner linked.     

Ein neues Praseodymniobat Pr2Nb11O30

A New Praseodymiumniobate Pr₂Nb₁₁O₃₀ By chemical vapor transport (T₂ → T₁, T₂ = 950 °C, T₁ = 900 °C, 3 d) of a mixture of PrOCl and Nb₂O₅ (1 : 1) using 5 mg NH₄Cl as transport agent we obtained the new compound Pr₂Nb₁₁O₃₀. The crystal structure determination [a = 6.2325(5) Å, c = 32.3677(36) Å, Z = 2, 1631 independent I₀, 69 parameters, R1 = 2.07%] shows CN = 8 (twofold capped octahedrally) for Pr, CN = 7 (pentagonal bipyramidally) for Nb(1,2) and CN = 6 (octahedrally) for Nb(3). The structure is closely related to that of Cu₅Ta₁₁O₃₀.     

Alkylidinphosphane und -arsane. I [P ≡ C?S]−[Li(dme)3]+ – Synthese und Struktur

Alkylidynephosphanes and -arsanes. I [P ≡ C? S]^?[Li(dme)₃]⁺ – Synthesis and Structure O,O′-Diethyl thiocarbonate and bis(tetrahydrofuran)-lithium bis(trimethylsilyl)phosphanide dissolved in 1,2-dimethoxyethane, react below 0°C to give ethoxy trimethylsilane and tris(1,2-dimethoxyethane-O,O′)lithium 2λ³-phosphaethynylsulfanide – [P≡C? S]^? [Li(dme)₃]⁺ – ( 1a ). Apart from bis(trimethylsilyl)sulfane or carbon oxide sulfide, dark red concentrated solutions of λ³-phosphaalkyne 1 are also obtained from reactions of carbon disulfide with bis(tetrahydrofuran)-lithium bis(trimethylsilyl)phosphanide or with the homologous lithoxy-methylidynephosphane ( 2 ) [1]. The ir spectrum shows two absorptions at 1762 and 747 cm^?1 characteristic for the P≡C and C? S stretching vibrations. The nmr parameters {δ(³¹P) ? 121.3; δ(¹³C) 190.8 ppm; ¹J_CP 18.2 Hz} resemble much more values of diorganylamino-2λ³-phosphaalkynes than those of bis(1,2-dimethoxyethane-O,O′)lithoxy-methylidyne-phosphane ( 2a ). As found by an X-ray structure analysis (P2₁/c; a = 1192.6(16); b = 1239.1(19); c = 1414.8(26) pm; β = 105.91(13)° at ?100 ± 3°C; Z = 4 formula units; wR = 0.064) of pale yellow crystals (mp. + 16°C) isolated from the reaction with O,O′-diethyl thiocarbonate, the solid is built up of separate [P≡C? S]^? and [Li(dme)₃]⁺ ions. Typical bond lengths and angles are: P≡C 155.5(11); C? S 162.0(11); Li? O 206.4(17) to 220.3(20) pm; P≡C? S 178.9(7)°.     

Ionenaustauschexperimente an ternären Tantalaten und Niobaten mittels Halogenidschmelzen — ein Zugang zu neuen Bleitantalaten

Exchange Reactions of Ternary Tantalates and Niobates with Halide Melts — a Way to New Lead Tantalates Ternary tantalates and niobates of the hexagonal structure-type A_(n+1)/m^m+M_3n+1O_8n+3 (A^m+ = Na⁺, Cu⁺, Ag⁺,…; M = Ta, Nb) were heated with surplus CuCl, PbCl₂, LaCl₃ or BiCl₃ (for example T = 700°C in case of PbCl₂). In some of these cases it was possible to exchange the A^m+-ions for the cations of the halide melts by maintaining the basic structure (for example: Cu₃Ta₇O₁₉ + BiCl₃ = BiTa₇O₁₉ + 3 CuCl). In different reactions the stack along the crystallographic c-axis and furthermore the proportion O/M (for example: 7 Cu₅Ta₁₁O₃₀ + 35/2 PbCl₂ = 11 Pb_1,5Ta₇O₁₉ + PbO + 35 CuCl) changed. Nevertheless, it was not possible to substitute cations of the halide melt for A^m+-ions in every direction (not possible for example: LaTa₇O₁₉ + BiCl₃). When CuCl? and PbCl₂-melt were added to Ag₂Ta₄O₁₁ and Na₂Nb₄O₁₁, these niobates showed exange reactions by changing their structure completely. If BiCl₃-melt was added, these niobates decayed while forming B? Nb₂O₅. The new hexagonal tantalates Pb_1,5Ta₇O₁₉ (a = 6,2411(7) Å; c = 19,977(3) Å) and PbTa₄O₁₁ (low-temperature modification; a = 6,2364(3) Å; c = 36,851(3) Å) were the first representatives of the structure-type A_(n+1)/m^m+M_3n+1O_8n+3 with A^m+ = Pb²⁺, which were found in a reaction with PbCl₂ (Cu₃Ta₇O₁₉ + 3/2 PbCl₂ = Pb_1,5Ta₇O₁₉ + 3 CuCl; Ag₂Ta₄O₁₁ + PbCl₂ = PbTa₄O₁₁ + 2 AgCl). These two compounds, which are probably metastable, could only be achieved by exange reactions of ions.     

Beiträge zur Kristallchemie und zum thermischen Verhalten von wasserfreien Phosphaten. XXXIII [1] In2P2O7, ein Indium(I)‐diphosphato‐indat(III) und In4(P2O7)3 — Darstellung,Kristallisation und Kristallstrukturen

Contributions on Crystal Chemistry and Thermal Behaviour of Anhydrous Phosphates. XXXIII [1] In₂P₂O₇ an Indium(I)‐diphosphatoindate(III), and In₄(P₂O₇)₃ — Synthesis, Crystallization, and Crystal Structure Solid state reactions via the gas phase lead to the new mixed‐valence indium(I, III)‐diphosphate In₂P₂O₇. Colourless single crystals of In₂P₂O₇ have been grown by isothermal heating of stoichiometric amounts of InPO₄ and InP (800 °C; 7d) using iodine as mineralizer. The structure of In₂P₂O₇ [P2₁/c, a = 7.550(1) Å, b = 10.412(1) Å, c = 8.461(2) Å, b = 105.82(1)°, 2813 independent reflections, 101 parameter, R1 = 0.031, wR2 = 0.078] is the first example for an In⁺ cation in pure oxygen coordination. Observed distances d(In^I‐O) are exceptionally long (d_min(In^I‐O) = 2.82 Å) and support assumption of mainly s‐character for the lone‐pair at the In⁺ ion. Single crystals of In₄(P₂O₇)₃ were grown by chemical vapour transport experiments in a temperature gradient (1000 → 900 °C) using P/I mixtures as transport agent. In contrast to the isostructural diphosphates M₄(P₂O₇)₃ (M = V, Cr, Fe) monoclinic instead of orthorhombic symmetry has been found for In₄(P₂O₇)₃ [P2₁/a, a = 13.248(3) Å, b = 9.758(1) Å, c = 13.442(2) Å, b = 108.94(1)°, 7221 independent reflexes, 281 parameter, R1 = 0.027, wR2 = 0.067].     

Ce2Ti2SiO9 – das erste Titanat‐Silicat mit Cer – Präparation,Charakterisierung und Struktur

Ce₂Ti₂SiO₉ – the First Titanate‐Silicate with Cerium – Preparation, Characterization, and Structure Ce₂Ti₂SiO₉ was synthesized by chemical vapour transport in a temperature gradient (1050 °C → 900 °C) using Ce₂Ti₂O₇ as precursor and ammoniumchloride as transport agent. SiO₂ was provided from the wall of the used silica tubes. The chemical composition of the crystals was determined by EDX and EELS analysis. The structure of Ce₂Ti₂SiO₉ was determined and refined to R1 = 0.025, _wR2 = 0.067, respectively. The monoclinic phase crystallizes in the space group C2/m (No. 12) with a = 16.907(3) Å, b = 5.7078(8) Å, c = 7.574(2) Å, β = 111.38(2)° and Z = 4. Ti is octahedral, Si is tetrahedral surrounded by oxygen. Ce(1) is coordinated by eight, Ce(2) by ten oxygen atoms. There are edge connected chains of Ti(1)–O‐octahedra parallel [010] which are connected along [001] with each other by Ti(2)–O‐octahedra‐pairs and Si–O‐tetrahedra.     

Beiträge zur Kristallchemie und zum thermischen Verhalten von wasserfreien Phosphaten. XXXVI [1] Synthese,Kristallstruktur und spektroskopische Charakterisierung von Palladium(II)‐diphosphat Pd2P2O7

Synthesis, Crystal Structure and Spectroscopical Characterization of Palladium(II)‐Diphosphate Pd₂P₂O₇ Pd₂P₂O₇ is synthesized by heating (T_max = 500 °C) stoichiometric amounts of PdO and phosphoric acid. Using chemical vapour transport experiments (850 °C → 750 °C, addition of PdCl₂) Pd₂P₂O₇ was crystallized. Pd₂P₂O₇ adopts its own structure type (C 2/c (No. 15), Z = 4, a = 13,151(2) Å, b = 5,172(1) Å, c = 8,139(1) Å, β = 97,52(1)°, 1160 independent reflections, 55 variables, R1 = 0,021 and wR2 = 0,050). Square‐planar [PdO₄]‐units are linked by diphosphate‐groups generating a 3D framework. Within this framework ribbons may be distinguished. Thus Pd₂P₂O₇ might be described as palladium(II)‐[diphosphatopalladate(II)]. The results of various spectroscopic measurements (IR, Raman, UV/VIS, ³¹P‐MAS‐NMR) are reported and discussed within the context of the crystal structure.     

Tribochemische und thermische Umwandlungen von LnTa3O9 (Ln = Pr,Nd) – röntgenographische und elektronenmikroskopische Untersuchungen

Tribochemical and Thermal Transitions of LnTa₃O₉ (Ln = Pr, Nd) — X-ray and Electron Microscopic Investigations Upon grinding crystals of M1? LnTa₃O₉ (Ln = Pr, Nd) [3] undergo a tribochemical phase transition. This leads to a new modifikation M2? LnTa₃O₉ with a significant higher density. We tried to find out more about the structure with high resolution electron microscopic investigations. According to electron diffraction and powder patterns the lattice parameters are (CuKα₁, λ = 1,54051 Å): M2? PrTa₃O₉: a = 6.2545(7) Å, b = 7.6736(7) Å, c = 6.5316(8) Å, β = 93.93(9)°; M2? NdTa₃O₉: a = 6.2552(5) Å, b = 7.6598(7) Å, c = 6.5103(4) Å, β = 94.096(7)°; (Z = 2). Using the intensities of powder patterns two structure models were calculated (space group P2₁/m, P2/m; R < 20%, heavy metal positions only). A through focus series of high resolution images was in better agreement with the first model (space group P2₁/m). Both models show a remarkable similarity to the structure of M? CeTa₃O₉ [4]. A thermal phase transition leads to M? PrTa₃O₉ and M? NdTa₃O₉ which are both isostructural to M? CeTa₃O₉.     

Synthese und Kristallstruktur des Fluorid‐ino‐Oxosilicats Cs2YFSi4O10

Synthesis and Crystal Structure of the Fluoride ino‐Oxosilicate Cs₂YFSi₄O₁₀ The novel fluoride oxosilicate Cs₂YFSi₄O₁₀ could be synthesized by the reaction of Y₂O₃, YF₃ and SiO₂ in the stoichiometric ratio 2 : 5 : 3 with an excess of CsF as fluxing agent in gastight sealed platinum ampoules within seventeen days at 700 °C. Single crystals of Cs₂YFSi₄O₁₀ appear as colourless, transparent and water‐resistant needles. The characteristic building unit of Cs₂YFSi₄O₁₀ (orthorhombic, Pnma (no. 62), a = 2239.75(9), b = 884.52(4), c = 1198.61(5) pm; Z = 8) comprises infinite tubular chains of vertex‐condensed [SiO₄]^4? tetrahedra along [010] consisting of eight‐membered half‐open cube shaped silicate cages. The four crystallographically different Si⁴⁺ cations all reside in general sites 8d with Si–O distances from 157 to 165 pm. Because of the rigid structure of this oxosilicate chain the bridging Si–O–Si angles vary extremely between 128 and 167°. The crystallographically unique Y³⁺ cation (in general site 8d as well) is surrounded by four O^2? and two F^? anions (d(Y–O) = 221–225 pm, d(Y–F) = 222 pm). These slightly distorted trans‐[YO₄F₂]^7? octahedra are linked via both apical F^? anions by vertex‐sharing to infinite chains along [010] (?(Y–F–Y) = 169°, ?(F–Y–F) = 177°). Each of these chains connects via terminal O^2? anions to three neighbouring oxosilicate chains to build up a corner‐shared, three‐dimensional framework. The resulting hexagonal and octagonal channels along [010] are occupied by the four crystallographically different Cs⁺ cations being ten‐, twelve‐, thirteen‐ and fourteenfold coordinated by O^2? and F^? anions (viz.[(Cs1)O₁₀]^19?, [(Cs2)O₁₀F₂]^21?, [(Cs3)O₁₂F]^24?, and [(Cs4)O₁₂F₂]^25? with d(Cs–O) = 309–390 pm and d(Cs–F) = 360–371 pm, respectively).     

Triorganoantimon- und Triorganobismutdisulfonate Kristall- und Molekülstrukturen von (C6H5)3M(O3SC6H5)2 (M = Sb,Bi)

Triorganoantimony and Triorganobismuth Disulfonates. Crystal and Molecular Structure of (C₆H₅)₃M(O₃SC₆H₅)₂(M = Sb, Bi) Triorganoantimony disulfonates R₃Sb(O₃SR′)₂ [R = CH₃ = Me, C₆H₅ = Ph; R′ = Me, CH₂CH₂OH, Ph, 4-CH₃C₆H₄. R = Ph; R′ = 2,4-(NO₂)₂C₆H₃], Me₃Sb(O₃SCF₃)₂ · 2 H₂O and triphenylbismuth disulfonates Ph₃Bi(O₃SR′)₂ [R = Me, CF₃, CH₂CH₂OH, Ph, 4-CH₃C₆H₄, 2,4-(NO₂)₂C₆H₃] have been prepared by reaction of Me₃Sb(OH)₂, (Ph₃SbO)₂, and Ph₃BiCO₃, respectively, with the appropriate sulfonic acids. From vibrational data an ionic structure is inferred for Me₃Sb(O₃SCF₃)₂ · 2 H₂O and Me₃Sb(O₃SCH₂CH₂OH)₂, and a covalent structure for the other compounds with a penta-coordinated central atom with trigonal bipyramidal surrounding (Ph or Me in equatorial, unidentate sulfonate ligands in apical positions). Ph₃M(O₃SPh)₂ (M = Sb, Bi) crystallize monoclinic [space group P2₁/c; M = Sb/Bi: a = 1 611.5(8)/1 557.4(9), b = 987.5(6)/1 072,5(8), c = 1 859.9(9)/1 696.5(9) pm, β = 105.71(5)/96.62(5)°; Z = 4; d(calc.) 1.556/1.781 Mg · m^?3; V_cell = 2 849.2 · 10⁶/2 814.8 · 10⁶ pm³; structure determination from 3 438/3 078 independent reflexions (I ≥ 3σ(I)), R(unweighted) = 0.030/0.029]. M is bonding to three Ph groups in the equational plane [mean distances Sb/Bi? C:210.1(4)/219.1(7) pm] and two sulfonate ligands with O in apical positions [distances Sb? O: 210.6(3), 212.8(2); Bi? O: 227.6(5), 228.0(4) pm]. Weak interaction of M with a second O atom of one sulfonate ligand is inferred from a rather short M? O contact distance [Sb? O: 327.4(4), Bi? O: 312.9(5) pm], and from the distortion of equatorial angles [C? Sb? C: 128.4(2), 119.2(2), 112.2(2); C? Bi? C: 135.9(3), 117.8(3), 106.3(3)°]     

Acyl- und Alkylidenarsane. VI. Vergleichende Untersuchungen zur Struktur von Bis (2,2-dimethylpropionyl) phenylarsan und -phosphan

Acyl- and Alkylidenearsines. VI. Comparative Studies on the Structures of Bis(2,2-di-methylpropionyl)phenylarsine and -phosphine . Bis(2,2-dimethylpropionyl)phenylarsine 1a [19] and -phosphine 1b [20] prepared from the corresponding bis(trimethylsilyl) derivative and 2,2-dimethylpropionyl chloride, crystallize in the monoclinic space group P2₁/c with following dimensions of the unit cell determined at a temperature of measurement of ?70 ± 3°C/?73 ± 3°C: a = 1449.3(7)/1468.3(3); b = 1050.0(5)/985.9(2); c = 1138.5(4)/1159.4(4) pm; β = 108.27(3)/105.61(3)°; Z = 4. X-ray structure determinations (R_w = 0.044/0.044) reveal distances of 205 and 191 pm between the pnicogen and the carbon atom of the carbonyl group which, as in similar trifluoromethyl compounds [2], are definitely elongated with respect to standard values of 194 and 183 pm. Further characteristic mean bond lengths and angles are: As? C(phenyl) 194; P? C(phenyl) 184; C?O 119/121; C(O)? C 153/154; C(O)? As? C(O) 91; C(O)? P? C(O) 95; As? C? O 120; P? C? O 120; As? C(O)? C 117 and P? C(O)? C 118°.     

Elektronenmikroskopische Untersuchung der Realstruktur von O?LaTa3O9, M?CeTa3O9 und M2?PrTa3O9 – Nachweis einer neuen M1?CeTa3O9-Modifikation

Electronmicroscopic Investigations on Disordered Crystals of O? LaTa₃O₉, M? CeTa₃O₉, and M2? PrTa₃O₉ – Proof of a New M1? CeTa₃O₉-Modification High resolution electron microscope investigations on O? LaTa₃O₉ and M2? PrTa₃O₉ showed twinned areas in both cases. With the help of electron microscopic pictures and models of the crystal structures, respectively, we obtained informations about the structural imperfections. Furthermore we present images of thin crystals which contain areas of two different modifications M1? PrTa₃O₉ and M2? PrTa₃O₉. By comparing these images with the corresponding computed contrasts we obtained a structure model of the phase boundary. Investigations on crystals of M? CeTa₃O₉ showed small areas of a new modification M1? CeTa₃O₉ which is isotypic to M1? LnTa₃O₉ (Ln=Pr, Nd) according to electron diffraction and high resolution images.