Crystal structure and fast ionic conduction of TIZrF5

TlZrF₅ crystallizes in the monoclinic system with unit cell dimensions a = 8.112(1) Å, b = 7.927(3) Å, c = 7.929(1) Å, β = 123.99(1)° and space group P2₁/c (n^o 14); Z = 4. The structure was solved by conventional Patterson and Fourier methods and refined by full-matrix least-squares techniques to a conventional R of 0.057 (R_ω = 0.063). The structure consists of sheets of (ZrF₅)^? that may be described as edge-shared and corner-shared bicapped trigonal prisms (ZrF₈). The sheets run parallel to the y0z plan and are bonded together by the Tl ions which are surrounded by 12 F^? ions. The ionic conductivity of TlZrF₅ and TlHfF₅ has been investigated by complex impedance measurements and the relationships between structure and fast-ionic conduction are discussed.     

Ionic mobility in ammonium-rubidium heptafluorozirconate (NH<Subscript>4</Subscript>)<Subscript>2.4</Subscript>Rb<Subscript>0.6</Subscript>ZrF<Subscript>7</Subscript> by (<Superscript>1</Superscript>H, <Superscript>19</Superscript>F) NMR data

NMR (¹⁹F, ¹H) methods are used to study ionic mobility in heptafluorozirconate (NH₄)_2.4Rb_0.6ZrF₇ in a range of temperatures from 150 K to 430 K. Types of ionic movements are determined, and their activation energy is evaluated. As a result of a phase transition a modification forms in which diffusion in the ammonium sublattice and isotropic reorientations of ZrF ₇ ^3? complex anions are observed. According to preliminary data, due to diffusion of ammonium ions the compound has relatively high ionic conductivity (σ ≈ 8.3 × 10^?5 S/cm at 423 K).     

Über Chalkogenolate. 102. Untersuchungen über Halbester der Monothiokohlensäure. 2. Kristallstruktur von Rubidiummethyloxoxanthat

On Chalcogenolates. 102. Studies on Hemiesters of Monothiocarbonic Acid. 2. Crystal Structure of Rubidium Methyl Oxoxanthate Rb[SOC? OCH₃] crystallizes with Z = 4 in the monoclinic space group P2₁/c with cell dimensions a = 4.332(3) Å, b = 11.349(5) Å, c = 10.673(5) Å, β = 92.9(5)°. The structure has been determined from single crystal X-ray data by means of Patterson and Fourier syntheses and refined to a final conventional R value of 0.045 using 983 independent reflexions. The structure consists of Rb⁺ and [SOC? OCH₃]^? ions. The rubidium ion is bonded to five oxygen and three sulfur atoms. The coordination polyhedron is a bicapped trigonal prism.     

New Heptafluorozirconates and ‐hafnates AIBIIZr(Hf)F7 (AI = Rb,Tl; BII = Ca,Cd) – Synthesis,Structures, and Structural Relationships

Four new ABZrF₇ heptafluorozirconates (A = Rb, Tl; B = Ca, Cd) and their homologous heptafluorohafnates, all colorless, orthorhombic Cmcm (n^o63), Z = 4, have been synthesized by heating stoichiometric mixtures of RbF or TlF, CaF₂ or CdF₂ and ZrF₄ (HfF₄) in sealed platinum tubes at temperature ranging from 550 °C (Tl) to 600 °C (Rb). The crystal structures of both RbCdZrF₇ and TlCdZrF₇ have been solved from single‐crystal X‐rays diffraction data. Rietveld refinements were performed from X‐rays powder patterns for RbCaZrF₇ and TlCaZrF₇. In this series of heptafluorides, both B²⁺ and Zr⁴⁺ cations exhibit a pentagonal bipyramidal 7‐coordination. Their structural relationships with other heptafluorozirconates A^IB^IIZrF₇ as well as β‐KYb₂F₇ are discussed. RbCaZrF₇: a = 6.863(1) Å, b = 11.130(1) Å, c = 8.485(1) Å; TlCaZrF₇: a = 6.868(1) Å, b = 11.165(1) Å, c = 8.486(1) Å; RbCdZrF₇: a = 6.780(1) Å, b = 11.054(4) Å, c = 8.420(4) Å; TlCdZrF₇: a = 6.784(3) Å, b = 11.099(2) Å, c = 8.424(9) Å.     

Zur Darstellung und Kristallstruktur von RbTlF4 und CsTlF4

Preparation and Crystal Structure of RbTlF₄ and CsTlF₄ RbTlF₄ and CsTlF₄ were synthesized by heating equivalent mixtures of alkaline chlorides or carbonates and Tl₂O₃ under a current of fluorine at 450–500°C. The crystal structure of RbTlF₄ has been determined by single crystal X-ray diffraction methods. The unit cell is orthorhombic with a = 8.252, b = 8.359, c = 6.244 Å (Z = 4); space group: C?Pb2₁a. CsTlF₄ and Tl^ITl^IIIF₄ (“TlF₂”) are isostructural with RbTlF₄. The structure contains layers of 2-dimensionally corner-linked distorted [TlF_4/2F₂]-octahedra, which are connected by rubidium ions.     

Mixed‐Valence Thallium(I,III) Bromides The Crystal Structure of α—Tl2Br3

Thallium sesquibromide Tl₂Br₃ is dimorphic. Scarlet coloured crystals of α‐Tl₂Br₃ were obtained by reactions of aqueous solutions of TlBr₃ and Tl₂SO₄ in agarose gel. In case of rapid crystallisation of hydrous TlBr₃/TlBr solutions and from TlBr/TlBr₂ melts ß‐Tl₂Br₃ is formed as scarlet coloured, extremely thin lamellae. The crystal structures of both forms are very similar and can be described as mixed‐valence thallium(I)‐hexabromothallates(III) Tl₃[TlBr₆]. In the monoclinic unit cell of α‐Tl₃[TlBr₆] (a = 26.763(7) Å; b = 15.311(6) Å; c = 27.375(6) Å; β = 108.63(2)°, Z = 32, space gr. C2/c) the 32 Tl^III‐cations are found in strongly distorted octahedral TlBr₆ groups. The 96 Tl^I cations are surrounded either by four or six TlBr₆ groups with contacts to 8 or 9 Br neighbors. Crystals of β‐Tl₃[TlBr₆] by contrast show almost hexagonal metrics (a = 13.124(4) Å, b = 13.130(4) Å, c = 25.550(7) Å, γ = 119.91(9)°, Z = 12, P2₁/m). Refinements of the parameters revealed structural disorder of TlBr₆ units, possibly resulting from multiple twinning. Both structures are composed of Tl₂[TlBr₆]^— and Tl₄[TlBr₆]⁺ multilayers, which alternate parallel (001). The structural relationships of the complicated structures of α‐ and β‐Tl₃[TlBr₆] to the three polymorphous forms of Tl₂Cl₃ as well as to the structures of monoclinic hexachlorothallates M₃TlCl₆ (M = K, Rb) and the cubic elpasolites are discussed.     

Syntheses and Crystal Structures of Rb2B2Se7, Tl2B2Se7, Cs3B3Se10, and Tl3B3Se10: New Perseleno‐selenoborates with Polymeric Anionic Chains

The perseleno‐selenoborates Rb₂B₂Se₇ and Cs₃B₃Se₁₀ were prepared from the metal selenides, amorphous boron and selenium, the thallium perseleno‐selenoborates Tl₂B₂Se₇ and Tl₃B₃Se₁₀ directly from the elements in evacuated carbon coated silica tubes by solid state reactions at temperatures between 920 K and 950 K. All structures were refined from single crystal X‐ray diffraction data. The isotypic perseleno‐selenoborates Rb₂B₂Se₇ and Tl₂B₂Se₇ crystallize in the monoclinic space group I 2/a (No. 15) with lattice parameters a = 12.414(3) Å, b = 7.314(2) Å, c = 14.092(3) Å, β = 107.30(3)°, and Z = 4 for Rb₂B₂Se₇ and a = 11.878(2) Å, b = 7.091(2) Å, c = 13.998(3) Å, β = 108.37(3)° with Z = 4 for Tl₂B₂Se₇. The isotypic perseleno‐selenoborates Cs₃B₃Se₁₀ and Tl₃B₃Se₁₀ crystallize in the triclinic space group P1 (Cs₃B₃Se₁₀: a = 7.583(2) Å, b = 8.464(2) Å, c = 15.276(3) Å, α = 107.03(3)°, β = 89.29(3)°, γ = 101.19(3)°, Z = 2, (non‐conventional setting); Tl₃B₃Se₁₀: a = 7.099(2) Å, b = 8.072(2) Å, c = 14.545(3) Å, α = 105.24(3)°, β = 95.82(3)°, γ = 92.79(3)°, and Z = 2). All crystal structures contain polymeric anionic chains of composition ([B₂Se₇]^2–)_n or ([B₃Se₁₀]^3–)_n formed by spirocyclically fused non‐planar five‐membered B₂Se₃ rings and six‐membered B₂Se₄ rings in a molar ratio of 1 : 1 or 2 : 1, respectively. All boron atoms have tetrahedral coordination with corner‐sharing BSe₄ tetrahedra additionally connected via Se–Se bridges. The cations are situated between three polymeric anionic chains leading to a nine‐fold coordination of the rubidium and thallium cations by selenium in M₂B₂Se₇ (M = Rb, Tl). Coordination numbers of Cs⁺ (Tl⁺) in Cs₃B₃Se₁₀ (Tl₃B₃Se₁₀) are 12(11) and 11(9).     

Preparation,Crystal Structure,Physical Properties,and Electronic Band Structure of TlTaS3

TlTaS₃ was prepared by applying a sequence of two melting processes with mixtures of Tl₂S, Ta, and S having different molar metal to sulphur ratios. TlTaS₃ crystallises in space group Pnma with a = 9.228(3)Å, b = 3.5030(6)Å, c = 14.209(3)Å, V = 459.3(2)ų, Z = 4. The structure is closely related to the NH₄CdCl₃‐type. Characteristic features of the structure are chains of edge‐sharing [Ta(+5)S₄S_2/2]₂ double octahedra running along [010]. These columns are linked by Tl⁺ ions. The Tl⁺ ion is surrounded by eight S^2— anions to form a distorted bi‐capped trigonal prism. The Tl⁺ ions are shifted from the centre of the trigonal prism toward one of the rectangular faces. This is discussed in context with other isostructural compounds. TlTaS₃ is a semiconductor. The electronic structure is discussed on the base of band structure calculations performed within the framework of density functional theory.     

Synthesis,spectroscopic and structural characterization of the first mixed fluoro-bromo group 4 organometallic complex [{Cp*ZrF2Br}4] (Cp* = C5Me5)

[{Cp*ZrF₂Br}₄] is conveniently prepared in high yield from the reaction of [{Cp*ZrF₃}₄] with four equivalents of Me₃SiBr. In contrast the reaction of [{Cp*ZrF₃}₄] with Me₃SiI under identical reaction conditions leads to a mixture of [Cp*ZrI₃] and unreacted [{Cp*ZrF₃}₄]. The crystal structure of [{Cp*ZrF₂Br}₄] has been determined by X-ray diffraction studies. The compound crystallizes in the orthorhombic crystal system [a = 9.325(1), b = 23.483(3), c = 27.016(5) Å, α = β = γ = 90°, space group Ibam, Z = 4]. The tetrameric core structure of [{Cp*ZrF₂Br}₄] contains four zirconium atoms linked by alternating single and triple fluorine bridges. One terminal bromine atom is bonded to each zirconium. ¹H and ¹⁹FNMR spectroscopic data and structural features of the title compound are compared with those for the mixed fluoro-chloro complexes [{Cp*ZrF₂Cl}₄], [{Cp*ZrF₂Cl}₂{Cp*ZrFCl₂}₂] and the trifluoro complex [{Cp*ZrF₃}₄].     

Synthesis and crystal structure of α-Ba2ZrF8 and Pb2ZrF8 determined ab initio from synchrotron and neutron powder diffraction data

α-Ba₂ZrF₈ is prepared as systematically twinned crystals by hydrothermal synthesis (200°C) or as fine powders either on a sand bath (60°C) (aqueous HF medium) or by solid state reaction at 450°C. Synchrotron radiation was used because of ambiguities in indexations from conventional X-ray (pseudo-hexagonal symmetry). The structure was determined ab initio from synchrotron powder data. Neutron data were used for improving accuracy because some degree of non-stoichiometry was suspected. The cell is orthorhombic, space group Prima, Z = 4, with a = 9.7401(1) Å, b = 5.6147(1) Å and c = 11.8871(1) Å (synchrotron data, 25°C). The final neutron Rietveld refinement led to R_P = 8.4 % and R_B = 3.5 % for the stoichiometric Ba₂ZrF₈ formulation (sand bath sample). The structure is built up from [ZrF₈] bicapped trigonal prisms isolated in a kinked fluorite matrix. The isostructural Pb₂ZrF₈ compound prepared in solution is also examined. An unexpected relationship with NaBaZrF₇ is discussed.     

Ionic mobility in heptafluorozirconantes with a mixed cationic sublattice as probed by <Superscript>1</Superscript>H and <Superscript>19</Superscript>F NMR

The ionic mobility in heptafluorozirconates (NH₄)_2.7Rb_0.3ZrF₇ and (NH₄)_2.75Cs_0.25ZrF₇ has been studied by ¹H and ¹⁹F NMR in the temperature range 150–430 K. The types of ion motion were determined and their activation energies were estimated. A phase transition results in a modification in which diffusion in the ammonium sublattice and orientational disorder of ZrF₇³⁻ anions are observed. Owing to diffusion of ammonium ions, the compounds have relatively high ionic conductivity (σ ≥ 5 × 10⁻⁵ S/cm at 420 K).     

Cristallochimie de TlIII6TeVIO12 et TlI6TeVIO6E6: un exemple original de l'activite´ste´re´ochimique de la pairee´lectronique 6s2(E) du thallium(I)

Both crystal structures of Tl₆TeO₁₂ and Tl₆TeO₆E₆ compounds have been determined, the former by X-ray single crystal techniques, the latter by powder neutron diffraction techniques. They crystallize in the trigonal system, space groupR3¯ the corresponding hexagonal cell parameters area = 9.645(2) Å,c = 9.421(2) Å, anda = 9.5722(3) Å,c = 9.3494(4) Å, respectively, withZ = 3. In both compounds tellurium(VI) is octahedrally coordinated to oxygen atoms with TeO distances of 1.936Åfor the Tl(III)-containing compound, i.e., Tl₆TeO₁₂, and 1.946Åfor Tl₆TeO₆ (Tl(I)). Tl(III) is surrounded by seven oxygen atoms sitting at the summits of a distorted monocapped trigonal prism. Tl(I) is linked to three oxygen atoms, forming a distorted TlO₃ pyramid. The lone pairs brought by Tl(I) are in the positions precedingly occupied by oxygen atoms in the crystal structure of Tl₆TeO₁₂. This is an outstanding example of the crystallochemical role of the lone pairsE which act like oxygen atoms, making Tl^I₆Te^VIO₆E₆ isostructural with Tl^IIITe^VIO₁₂. Structural relationships with fluorite type network are discussed.     

Ionic mobility and structure of glasses in Zrf<Subscript>4</Subscript>—Bif<Subscript>3</Subscript>—Mf<Subscript>2</Subscript> (M = Sr,Ba, Pb) systems according to Nmr,Ir, and Raman spectroscopic data

The NMR (¹⁹F and MAS NMR ¹⁹F), IR, and Raman spectroscopic methods are used to study the ionic mobility and structure of a series of new glasses in ZrF₄—BiF₃—MF₂ (M = Sr, Ba, Pb) systems in a temperature range of 180 K to 500 K. The temperature range, in which diffusion of fluorine ions becomes the dominant form of ionic motion, is determined by the nature of the M₂+ cation. The factors determining the basic model of the structure of glasses in ZrF₄—BiF₃—MF₂ (M = Sr, Ba, Pb) systems and conditions under which bismuth polyhedra can participate in the construction of the glass network are considered. According to the data of impedance spectroscopy, the studied glasses have relatively high ionic conductivity (δ ≥ 10–₄ S/cm above 480 K).     

Über ein neues Erdalkalioxothallat: Sr4Tl2O7

On a Novel Alkaline Earth Metal Oxothallate: Sr₄Tl₂O₇ The hitherto unknown compound Sr₄Tl₂O₇ was prepared and investigated by X-ray single crystal methods. Sr₄Tl₂O₇ crystallizes in the tetragonal space group C? P4₂nm (a = 5.006, c = 18.73 Å). Sr²⁺ has a trigonal prismatic surrounding whereas Tl³⁺ shows 2+2 oxygen neighbours. The crystal structure is completely described.     

Crystal Structure and Ionic Conductivity of Cesium Trifluoromethyl Sulfonate,CsSO3CF3

The crystal structures of the room and the high temperature modifications of cesium trifluoromethyl sulfonate were solved from high resolution X‐ray powder diffraction data. At room temperature, α‐CsSO₃CF₃ crystallizes in the monoclinic space group P2₁ with lattice parameters a = 9.7406(2) Å, b = 6.1640(1) Å, c = 5.4798(1) Å, and β = 104.998(1)°; Z = 2. At temperatures above T = 380 K, a second order phase transformation towards a disordered C‐centered orthorhombic phase in space group Cmcm occurs with lattice parameters at T = 492 K of a = 5.5074(3) Å, b = 19.4346(14) Å, and c = 6.2978(4) Å; Z = 4. Within the crystal structures, the triflate anions are arranged in double layers with the apolar CF₃‐groups pointing towards each other. The cesium ions are located between the SO₃‐groups. CsSO₃CF₃ shows a specific ion conductivity ranging from σ = 1.06·10^?8 Scm^?1 at T = 393 K to σ = 5.18·10^?4 Scm^?1 at T = 519 K.     

2-Hydroxy-4-methylbenzenesulfonic acid dihydrate: Crystal structure, vibrational spectra, proton conductivity, and thermal stability

The crystal and molecular structure of 2-hydroxy4-methylbenzenesulfonic acid dihydrate C₆H₃(CH₃)(OHSO^? ₃ H₅O₂ ⁺ (I) was studied by X-ray diffraction and vibrational spectroscopy. The compound crystallized in the monoclinic crystal system; crystal data: a=10.853(2) Å, b=7.937(2) Å, c=12.732(3) Å, β=112.13(3)°, V=1015.9(4)ų,Z=4,d_calc=1.466g/cm³,spacegroupP2₁/c,R_f=0.0486,GOOF=1.161.The S-O distances in the sulfonate group differed substantially (S1-O2 1.439(2) Å, S1-O3 1.455(2) Å, and S1-O4 1.464(2) Å. The symmetry of the H₅O₂ cation decreased due to proton displacement toward one of the two water molecules. XRD data on the asymmetry of H5O2 were confirmed by IR and Raman spectral data. The strong triplet at 2900, 3166, 3377 cm^?1 in the IR spectrum of I corresponds to different types of H-bond and shifted to 2185, 2363, 2553 cm^?1 after deuteration. The proton conductivity of the compound was measured by impedance spectroscopy: 6 × 10^?7 S/cm at 298 K (32 rel %), E _act=0.4±0.01 eV. The conductivity increased to 10^-3 S/cm, E_act=0.1 eV when ambient humidity increased to 60 rel %.     

Synthesis,Characterization, Structural and Theoretical Analysis of a New Rare‐Earth Boride Carbide: Lu3BC3

Lu₃BC₃ is prepared by arc‐melting of the elements. The silver colored compound crystallizes in the space group Cmcm (Z = 4, a = 4.9788(3) Å, b = 5.0109(3) Å, c = 15.669(1) Å). The crystal structure contains discrete carbon atoms and CBC units in octahedra and bicapped cubes of metal atoms, respectively. The structural analysis is consistent with the group oxidation states (Lu³⁺)₃(C^4–)(CBC^5–). Extended Hückel and LAPW calculations have been performed. Although a semiconducting behavior could be anticipated, the valence band and the conduction band are touching according to LAPW calculations in agreement with the observed metallic conductivity of the compound.     

Crystal structure of (glycine) sodium nitrate Gly·NaNO3

The crystal structure of Gly·NaNO₃ was determined by single crystal diffraction methods (monoclinic crystal system, B11n, a = 14.339(3) Å, b = 9.136(3) Å, c = 5.263(3) Å, γ = 119.14(5)°). The structure is built from alternating layers of glycine organic molecules and inorganic layers consisting of Na⁺ ions and planar NO ₃ ^? ions stretching along the b axis. The surroundings of the Na atom include the oxygen atoms of the NO ₃ ^? groups and the oxygen atoms of glycine molecules. The structure has a system of hydrogen bonds.     

Zur Darstellung und Kristallstruktur von Tl2O

The preparation of Tl₂O and its crystal structure is discussed. By FOURIER methods for a monoclinic unit cell(a_M = 6.08₂, b_M = 3.52₀, c_M = 13.2₄ Å, β = 108.2°, Z = 4, space group C_2h³) the determined atomic parameters can be transformed into the trigonal system by the assumption of special oxygen positions (space group No. 166–R3 m). Correspondingly the Tl₂O crystal structure may be described as a threefold polytype form of the anti CdJ₂ type (a_H = 3,51₆ c_H = 37.8₄ Å; c/a = 10.76, Z = 6, mol. vol. = 40.7 cm³; d_x = 10.44, d_pyk = 10.4 g m^?).