Die H-Phasen: Ti2CdC,Ti2GaC,Ti2GaN,Ti2InN,Zr2InN und Nb2GaC

Zusammenfassung Die ternären Phasen Ti₂CdC, Ti₂GaC, Ti₂GaN, Ti₂InN, Zr₂InN und Nb₂GaC werden aus Monocarbid bzw.-nitrid, Übergangsmetall und Metametall hergestellt. Die Verbindungen erweisen sich sämtlich mit Cr₂AlC (H-Phase) isotyp. Die Gitterparameter werden ermittelt.     

Die H-Phasen Ti2InC,Zr2InC,Hf2InC und Ti2GeC

Zusammenfassung Die Doppelcarbide Ti₂InC, Zr₂InC, Hf₂InC und Ti₂GeC werden hergestellt und kristallchemisch als H-Phasen identifiziert.     

Dielectric properties of chemically co-precipitated tetragonal Pb(Mg1/3Nb2/3)0.65Ti0.35O3

Pyrochlore phase free Pb(Mg_1/3Nb_2/3)_0.65Ti_0.35O₃ ceramics have been synthesized successfully by chemical co-precipitation method. It has been noted that formation of perovskite phase Pb(Mg_1/3Nb_2/3)_0.65Ti_0.35O₃ without pyrochlore phase is tricky. The synthesized samples at optimized parameters were characterized using X-ray diffraction technique. Careful analysis of the XRD data predicts the tetragonal lattice structure. The morphological studies depict the presence of uniform grain size. Dielectric constant (ε′) and loss tangent (tan δ), at and well above room temperature, were studied. The variation of dielectric constant with temperature shows sharp peak at ferroelectric–paraelectric transition temperature. Further, the temperature dependent dielectric constant shows good fit with modified Curie–Weiss law, which suggests normal ferroelectric behavior of Pb(Mg_1/3Nb_2/3)_0.65Ti_0.35O₃.     

Crystal Structure of BaNb6.3(1)Ti3.6(1)O16 containing Nb6O12, fused Ti3O13 Clusters and Ti3O10 Units

A new phase, BaNb_6.3(1)Ti_3.6(1)O₁₆, has been synthesised. Electron diffraction studies indicate an hexagonal substructure with unit cell parameters a ≈ 8.9 Å and c ≈ 9.5 Å. In some of the ED patterns superstructure reflections are present, indicating a supercell with a = √3 · a_sub and c = c_sub. However, X‐ray single‐crystal diffraction studies of a crystallite yielding reflections corresponding to the supercell revealed it to be monoclinic, with the unit cell parameters a = 26.811(2) Å, b = 15.4798(2) Å, c = 9.414(2) Å, β = γ = 90° and α = 90.0(3)°. The average crystal structure was refined, using the subcell with a = 8.937(2) Å, b = 15.479(2) Å, c = 9.414(2) Å, β = γ = 90° and α = 90.0(3)°, space group Cm11, and Z = 4, to R_I = 3.24% and R_wI = 3.44%. The structure can be described as an hexagonal close packing layers of Nb₆ octahedra, Ba, and O atoms (A1, A2) and layers of O atoms (B1, B2), appearing in the packing sequence: A1B1A2B2. The Nb₆ octahedra are found in isolated Nb₆O₁₂O₆ clusters, and the Ti atoms in Ti₃O₁₃ and Ti₃O₁₀ units in octahedral and tetrahedral voids formed by O atoms, respectively. The Ti positions were found to be only partly occupied. Microanalysis indicates that some Nb atoms are located in the Ti₃ triangles. A model is presented that interprets these not fully occupied Ti₃ triangles as a result of a superimposing of three different structures. Two of these consist of two fused Ti₃O₁₃ units, forming an Ti₆O₁₉ unit, and a Ti₃O₁₀ unit, while the third consists of alternating Ti₃O₁₃ units.     

Magnetische Eigenschaften von Ti3−xMxO5-Phasen (M = V3+, Cr3+, Nb4+)

Magnetic Properties of Ti_3?xM_xO₅ Phases (M = V³⁺, Cr³⁺, Nb⁴⁺) The magnetic properties of Ti_3?xV_xO₅, Ti_3?xCr_xO₅, and Ti_3?xNb_xO₅ phases are reported. In the case of V³⁺ and Cr³⁺ the magnetic leaping-temperature decreases, however Nb⁴⁺ shift the phase-transition towards higher temperatures. All samples show a “memory-effect” in magnetic properties, i. e. the results of heating- and cooling-cycles are higher susceptibilities of the α-phase of Ti₃O₅. Endowed Ti₃O₅ phases show for the α- and β-Ti_3?xM_xO₅ til the leap Curie-Weiss characteristic in 1/X vs. temperature measurements. Exception is β-Ti_3?xNb_xO₅, its susceptibility is independend of the temperature up to x ? 0.3.     

Theoretical studies on redox properties,protonation sites,and electronic spectrum of a new type of polyoxometalate [Ti12Nb6O44]10− by DFT

The electronic structure of a new type of polyoxometalate [Ti₁₂Nb₆O₄₄]^10? has been investigated using density functional theory (DFT). The calculations represent that the LUMO in fully oxidized [Ti₁₂Nb₆O₄₄]^10? delocalizes among the titanium (Ti) and niobium (Nb). Therefore, both Ti and Nb have the probability to accept extra electron when [Ti₁₂Nb₆O₄₄]^10? as catalyst is reduced, which has been reinforced by the spin density for the monoreduced specie [Ti₁₂Nb₆O₄₄]^11?. Three kinds of possible protonated isomers [HTi₁₂Nb₆O₄₄]^9? are discussed. The results reveal that the preferred protonation sites correspond to bridging oxygens Nb? O? Ti. In addition, the calculation of electronic spectrum shows that there is an obvious intramolecular charge transfer from oxygen to metal. The solvent effects were also considered in the calculations by using a conductor‐like screening model (COSMO) of solvation with the solvent‐excluding surface. © 2009 Wiley Periodicals, Inc. Int J Quantum Chem, 2009     

Die Kristallstruktur von Ti3InC,Ti3InN,Ti3TIC und Ti3TIN

Zusammenfassung Die ternären Phasen Ti₃InC, Ti₃InN, Ti₃TIC und Ti₃TIN werden aus TiC (TiN) und den metallischen Komponenten hergestellt. Diese Verbindungen sind mit den Perowskit-Carbiden (-Nitriden) isotyp.     

The oxychlorides in Nb6 cluster chemistry

The Nb₆ oxychlorides based on Nb₆L₁₈ units that we have isolated, as well as another one recently reported in the literature, are reviewed. Each of them is structurally described through a relevant example: Cs₂LuNb₆Cl₁₇O, Cs₂UNb₆Cl₁₅O₃, ScNb₆Cl₁₃O₃, Ti₂Nb₆Cl₁₄O₄ and KLu₃Nb₆Cl₁₅O₆, the structure of the latter has just been solved. They are discussed by comparison with the Nb₆ chlorides and Nb₆ oxides, considering the electronic and steric evolution of the Nb₆L₁₈ unit upon increasing O/C1 ratio. The environments of the trivalent cations will be compared, specially those involving extra halogens in KLu₃Nb₆Cl₁₅O₆ and Ti₂Nb₆Cl₁₄O₄.     

Quantitative WDXS Microanalysis of Bismuth-Based BaBi4Ti4O15 Perovskites Doped with Nb and Fe

 Quantitative electron-probe microanalysis was used to determine the chemical composition of an Fe- and Nb-doped bismuth-based BaBi₄Ti₄O₁₅ perovskite compound. Elemental concentrations of Fe, Nb, Bi, Ba and Ti were accurately measured using wavelength-dispersive X-ray spectroscopy that was optimised for the analysis of a complex oxide matrix containing minor concentrations of dopants. Measurements were performed with a JEOL JXA 840A electron probe microanalyser at 20 and 26 kV, 50 nA beam current, 100 s maximum counting time and 0.3% preset counting deviation (σ_c) using both PET and LiF crystals. K-ratios were quantified by the ZAF and the φ(ρz) PAP matrix-correction procedures. The results showed that dopants incorporate into the BaBi₄Ti₄O₁₅ at Ti^4 + sites according to the Ba_1−4XBi_4 + 4XTi_4−4XFe_4XO₁₅ and Ba_1 + 4XBi_4−4XTi_4−4XNb_4XO₁₅ solid-solution formulae. The majority of the excess charge introduced by the substitution of Ti^4 + with Fe^3 + or Nb^5 + is compensated for the change in the Ba^2 +/Bi^3 + ratio.     

Pyrochlore formation, phase relations, and properties in the CaO-TiO2-(Nb,Ta)2O5 systems

Phase equilibria studies of the CaO:TiO₂:Nb₂O₅ system confirmed the formation of six ternary phases: pyrochlore (A₂B₂O₆O′), and five members of the (110) perovskite-slab series Ca_n(Ti,Nb)_nO_3n+2, with n=4.5, 5, 6, 7, and 8. Relations in the quasibinary Ca₂Nb₂O₇−CaTiO₃ system, which contains the Ca_n(Ti,Nb)_nO_3n+2 phases, were determined in detail. CaTiO₃ forms solid solutions with Ca₂Nb₂O₇ as well as CaNb₂O₆, resulting in a triangular single-phase perovskite region with corners CaTiO₃-70Ca₂Ti₂O₆:30Ca₂Nb₂O₇-80CaTiO₃:20CaNb₂O₆. A pyrochlore solid solution forms approximately along a line from 42.7:42.7:14.6 to 42.2:40.8:17.0 CaO:TiO₂:Nb₂O₅, suggesting formulas ranging from Ca_1.48Ti_1.48Nb_1.02O₇ to Ca_1.41Ti_1.37Nb_1.14O₇ (assuming filled oxygen sites), respectively. Several compositions in the CaO:TiO₂:Ta₂O₅ system were equilibrated to check its similarity to the niobia system in the pyrochlore region, which was confirmed. Structural refinements of the pyrochlores Ca_1.46Ti_1.38Nb_1.11O₇ and Ca_1.51Ti_1.32V_0.04Ta_1.10O₇ using single-crystal X-ray diffraction data are reported (Fd3m (#227), a=10.2301(2) Å (Nb), a=10.2383(2) Å (Ta)), with Ti mixing on the A-type Ca sites as well as the octahedral B-type sites. Identical displacive disorder was found for the niobate and tantalate pyrochlores: Ca occupies the ideal 16d position, but Ti is displaced 0.7 Å to partially occupy a ring of six 96g sites, thereby reducing its coordination number from eight to five (distorted trigonal bipyramidal). The O′ oxygens in both pyrochlores were displaced 0.48 Å from the ideal 8b position to a tetrahedral cluster of 32e sites. The refinement results also suggested that some of the Ti in the A-type positions may occupy distorted tetrahedra, as observed in some zirconolite-type phases. The Ca-Ti-(Nb,Ta)-O pyrochlores both exhibited dielectric relaxation similar to that observed for some Bi-containing pyrochlores, which also exhibit displacively disordered crystal structures. Observation of dielectric relaxation in the Ca-Ti-(Nb,Ta)-O pyrochlores suggests that it arises from the displacive disorder and not from the presence of polarizable lone-pair cations such as Bi³⁺.     

Perovskite related phases in the Sr5Nb4O15 - SrTiO3 - Sr4Nb2O9 system

Phase relations have been investigated within the Sr₅Nb₄O₁₅−SrTiO₃−Sr₄Nb₂O₉ region of the SrO−Nb₂O₅−TiO₂ system with a view to clarifying the occurrence of fully oxidised perovskite related phases. Overall phase analysis was carried out by powder X-ray diffraction and microstructures were clarified by transmission electron microscopy. There is only one main composition triangle in this area at 1350°C. The tie-line between Sr₅Nb₄O₁₅ and SrTiO₃ contains a homologous series of hexagonal layered perovskite phases including Sr₆Nb₄TiO₁₈ and Sr₇Nb₄Ti₂O₂₁. The phase Sr₄Nb₂O₉ is a nonstoichiometric phase with a disordered perovskite structure. There is some extension of this phase along the Sr₄Nb₂O₉−SrTiO₃ tie-line, but SrTiO₃ does not show a significant composition range. Samples with a composition Sr₄Nb₂O₉, when heated at 900°C show several ordered modifications. Samples along the Sr₄Nb₂O₉−SrTiO₃ tie-line which are annealed at 900°C contain these ordered materials together with samples showing considerable short range order which increases as the Ti content increases.     

Transparent thin films of Bi2WO6, Bi4Ti3O12 and Sr0.75Ba0.25Nb2O6

Transparent thin films were prepared by a sol–gel method starting from precursor formation in solution, subsequent spin coating followed by a heating ramp up to a maximum of 700 °C. Starting from a Bi₂MoO₆ synthesis route, the phase formation and thin film processing of the bismuth containing materials Bi₂WO₆, Bi₃Ti₄O₁₂ and additionally of the tungsten–bronze structure Sr_0.75Ba_0.25Nb₂O₆ were studied. Spin coating was used to adjust the film thickness in a wide range from 6 to 200 nm. All films were obtained as multicrystalline pure phases according to X-ray diffraction analyses. Scanning electron micrographs revealed homogeneous coatings composed of nanoparticles with a crystallite size varying between 20 and 100 nm, furthermore the UV–VIS spectra demonstrated a high transparency of the films, 80–90% at 600 nm.     

Na3Al2Nb34O64 und Na (Si,Nb) Nb10O19: Clusterverbindungen mit isolierten Nb6-Oktaedern

Na₃Al₂Nb₃₄O₆₄ and Na (Si, Nb) Nb₁₀O₁₉. Cluster Compounds with Isolated Nb₆-Octahedra Hexagonal ormolu coloured plates of the new compounds Na₃Al₂Nb₃₄O₆₄ ( I ) and Na(Si, Nb)Nb₁₀O₁₉ ( II ) were prepared by heating pellets of NaF, Al₂O₃, NbO₂ and NbO (3:1:8:2) and NaF, NbO₂ and NbO (1:4:2), respectively, at approx. 850°C. I was contained in a sealed gold capsule, II in a silica tube. The Si incorporated in II originates from the container material. Both compounds crystallize in R 3 , I with a = 784.4(1), c = 7065(1) pm, Z = 3 and II with a = 784.1(1), c = 4221.8(5) pm, Z = 6. I and II represent new structure types. They contain the same characteristic structural units, namely discrete Nb₆O₁₂ clusters (d_Nb–Nb = 283 ± 4 pm) and Nb₂O₁₀ units with Nb–Nb dumbells (d_Nb–Nb ≈? 269 pm) in edgesharing coordination octahedra. In addition NbO₆ octahedra containing Nb in the oxidation state + 5 and NaO₁₂ cube-octahedra occur in both compounds besides AlO₄ and SiO₄ tetrahedra in I and II , respectively. The structures can be described in terms of a common closepacking of O and Na atoms together with Nb₆ octahedra.     

Ein Beitrag über Oxide vom Typ AMO4 (A = Ti3+, Cr3+; M = Nb5+, Ta5+)

A Contribution on Ternary Oxides of the AMO₄-Type (A = Ti³⁺, Cr³⁺; M = Nb⁵⁺, Ta⁵⁺ ) CrNbO₄, CrTaO₄, TiNbO₄, and TiTaO₄ were prepared by CO₂-laser technique. X-ray single crystal investigations show a random distribution of the metal ions in Rutil type structure, space group D–P4₂/mnm. Calculations of the free energy of reaction between Ti₂O₃ and Nb₂O₅ show higher stability of TiO₂ beside NbO₂. In TiNbO₄ both metals exhibit the oxidation state +4.     

Nb2Y2X6, a Novel Type of NbIV Compounds with Cross-linked Nb2 and Y2 Dumbbells (Y = Se,Te; X = Br,I)

The compounds Nb₂Se₂Br₆, Nb₂Te₂Br₆, and Nb₂Te₂I₆ were prepared from the elements in sealed quartz ampoulès at 1073 K. The crystalline solids, exhibiting a metallic lustre, are insensitive against moisture and oxygen. All compounds undergo several reversible thermal transitions with temperature (DTA). Beside binary halides only NbYX₃ is present in the gas phase. The structures consist of one-dimensional infinite chains of halogen bridged Nb₂(Y₂)X₄ units containing single side-on bonded Nb₂ and Y₂ dumbbells forming a quasi tetrahedral Nb₂Y₂ cluster (Nb? Nb ? 283.2; 287.5; 293.2 pm; Se? Se ? 230.5 pm; Te? Te ? 267.0; 268.5 pm). The structural and magnetic properties clearly prove the formal oxidation states Nb⁴⁺ and Y^1?, unexpected from stoichiometry. (Structural data: all P2/a (No. 13); Nb₂Se₂Br₆: a = 1254.0(12); b = 689.7(10); c = 662.4(10) pm; β = 98.9(1)°; Z = 2; 1274 hkl; R = 0.066. Nb₂Te₂Br₆: a = 1259.7(13); b = 713.5(9); c = 667.0(9) pm; β = 97.6(1)°; 1557 hkl; R = 0.043. Nb₂Te₂I₆: a = 1347.3(3); b = 742.9(2); c = 714.1(2) pm; β = 98.52(2)°; 1540 hkl; R = 0.026).     

Die Phasen Nb3Ga2, Ta5Ga3 und Ta5Al3Bx

Zusammenfassung Die Phasen Nb₃Ga₂, Ta₅Ga₃ und Ta₅Al₃B_x werden aus den Komponenten hergestellt. Nb₃Ga₂ kristallisiert im U₃Si₂-Typ, Ta₅Ga₃ hat Cr₅Br₃-Struktur (T 2) und Ta₅Al₃B_x ist mit Mn₅Si₃ (teilweise aufgefüllt) isotyp.     

Die Kristallstruktur von Ti3SiC2—ein neuer Komplexcarbid-Typ

Zusammenfassung Die Struktur von Ti₃SiC₂ wird aus Einkristallaufnahmen bestimmt. Die Gitterparameter der hexagonalen Zelle sind:a=3,06₈,c=17,66₉ Å undc/a=5,75₉. Die Titan-Atome besetzen die Punktlagen 2a) und 4f) (z_Ti=0,135), die Silicium-Atome die Punktlage 2b) und die Kohlenstoff-Atome die Punktlage 4f) (z_C=0,567₅) in der Raumgruppe D _6h ⁴ –P6₃/mmc. Die Struktur gehört zu den Komplexcarbiden mit oktaedrischen Bauelementen [T ₆C].

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The crystal structure of Ti₃SiC₂ has been determined by means of single crystal photographs; the lattice parameters of the hexagonal cell were found to be:a=3.06₈,c=17.66₉ Å andc/a=5.75₉. The titanium atoms occupy the positions 2a) and 4f) (z_Ti=0.135), the silicon atoms 2b) and the carbon atoms 4f) (z_C=0.567₅) of the space group D _6h ⁴ –P6₃/mmc. The crystal structure type belongs to the class of complex carbides having octahedral groups [T ₆C].

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Mit 5 Abbildungen     

Die Kristallstruktur von Nb5Cu4Si4

Zusammenfassung Die Struktur von Nb₅Cu₄Si₄ wird mit Hilfe von Einkristallmethoden bestimmt und verfeinert. Die Abmessungen der tetragonalen, innenzentrierten Elementarzelle sind:a=10,1908 undc=3,6004 Å. Die Zelle beinhaltet 2 Formeleinheiten, die Raumgruppe ist C _4h ⁵ –I4/m.

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The crystal structure of Nb₅Cu₄Si₄ has been determined and refined by single-crystal X-ray methods. The cell dimensions of the tetragonal body-centered unit cell are found to be:a=10,1908 andc=3,6004Å. The cell content is 2 formula units, the space group is C _4h ⁵ –I4/m.

     

Darstellung und Kristallstruktur der Pnictidoxide Na2Ti2As2O und Na2Ti2Sb2O

Preparation and Crystal Structure of the Pnictide Oxides Na₂Ti₂As₂O and Na₂Ti₂Sb₂O Na₂Ti₂As₂O and Na₂Ti₂Sb₂O were synthesized in form of very easily hydrolysed metallic-grey powders by reaction of Na₂O and TiAs resp. TiSb in sealed tantalum tubes under argon. The tetrahedral bodycentered crystallizing compounds from a modified anti-K₂NiF₄ structure type [1] (also called Eu₄As₂O-type [2,3]), space group I4/mmm (no. 139), with the lattice constants for Na₂Ti₂As₂O: a = 407.0(2) pm, c = 1528.8(4) pm and for Na₂Ti₂Sb₂O: a = 414.4(0) pm, c = 1656.1(1) pm. Magnetic measurements of powder samples of Na₂Ti₂Sb₂O show antiferromagnetic interaction within the Ti—O-layers. Superconductivity was not found by ac-shielding method down to 4 K.     

Formation of rutile-type Nb0.94O2 by shock reduction of Nb2O5

Shock-recovery experiments on Nb₂O₅ powder specimens are made in pressure ranges up to 50 GPa using the gun method. “NbO₂” with the rutile structure is formed above about 40 GPa when an open recovery fixture is used. The tetragonal unit cell dimensions are measured to be a = 4.784(2) Å, c = 3.029(2) Å, and V = 69.34(6) ų. The metal-to-oxygen ratio is determined to be Nb_0.94O₂ by means of thermogravimetry. A comparative study is made on the shock reduction behavior of Nb₂O₅ and Ta₂O₅.