Zur Atomverteilung in Ba2SrIn2O6 mit einem Beitrag zur Existenz des Calciumferrat(III)-Typs bei Oxoindaten

On the Atomic Distribution in Ba₂SrIn₂O₆ with a Contribution to the Existence of the Calciumferrite-Type of Oxoindates (I) Ba₂SrIn₂O₆ and (II) Sr_0.93Ba_0.07In₂O₄ were prepared and investigated by single crystal X-ray technique. I crystallizes with tetragonal symmetry, space group D – I4/mmm, a = 4.168; c = 21.290 Å; Z = 2; II belongs to the orthorhombic space group D – Pnma, a = 9.858; b = 3.273; c = 11.520 Å; Z = 4. I shows in respect to the formerly investigated compound BaSr₂In₂O₆ an unexpected statistically distribution of Ba²⁺ and Sr²⁺ with the La₂SrCu₂O₆ type. II marks the range of existence of the calciumferrite type within the alkaline earth oxoindates in direction of large radii of M²⁺ ions.     

Ein Beitrag über CuPrMo2O8 und CuTbMo2O8

A Contribution on CuPrMo₂O₈ and CuTbMo₂O₈ Single crystals of (I): CuPrMo₂O₈ and (II): CuTbMo₂O₈ were prepared by solid state reactions in closed copper tubes. They crystallize with orthorhombic symmetry, space group D-Pbca, (I): a = 10.4114, b = 9.8917, c = 14.8287 Å, (II): a = 10.2243, b = 9.7385, c = 14.6000, Z = 8. Both compounds are isotypic to CuYMo₂O₈, showing isolated MoO₄ tetrahedra, square antiprismatic coordination of Ln³⁺ and Cu⁺ besides one edge of an O^2? triangle. Calculations of the coulombterm of lattice energy support the oxidation state Cu²⁺ in combination with mixed valences of Mo⁶⁺ and Mo⁵⁺ on the molybdenum point positions.     

Hochdrucksynthese von BaSr2P6N12 und BaCa2P6N12 und Strukturvergleich der Reihe BaP2N4, BaCa2P6N12 und BaSr2P6N12

High‐Pressure Synthesis of BaSr₂P₆N₁₂ and BaCa₂P₆N₁₂ and Comparison of the Structures of BaP₂N₄, BaCa₂P₆N₁₂, and BaSr₂P₆N₁₂ The novel nitridophosphates BaCa₂P₆N₁₂ and BaSr₂P₆ N₁₂ were obtained by means of high‐pressure high‐temperature synthesis utilizing the multianvil technique (1200 °C, 5 GPa). The complex anion [PN₂^?] of the title compound is formally isoelectronic with silica. The crystal structure was solved from powder data and refined by the Rietveld method (BaCa₂P₆N₁₂: , Z = 4, a = 9,9578(2) Å; BaSr₂P₆N₁₂: , Z = 4, 10,0705(2) Å). The crystal structures are derived from that of BaP₂N₄ which is isotypic with a high pressure phase of CaB₂O₄ and BaGa₂S₄. For each compound the ³¹P solid state NMR spectrum yielded a single resonance (BaCa₂P₆N₁₂: 7.4 ppm; BaSr₂P₆N₁₂:3.9 ppm).     

Zur Kenntnis von SrCa2In2O6

About SrCa₂In₂O₆ The hitherto unknown compound SrCa₂In₂O₆ was investigated by X-ray single crystal methods (a = 1 104.6, b = 1 663.0, c = 327.9 pm, space group D—Pbam). SrCa₂In₂O₆ is isotypic with Ca₃In₂O₆, but it will be shown that Ca₂In₂O₆ may be a special case of the polyhedral occupation of the SrCa₂In₂O₆ structure.     

Synthese und Untersuchung von NiNb2O6-Einkristallen mit Columbit- und Rutilstruktur

Synthesis and Investigation of NiNb₂O₆ Single Crystals of Columbite and Rutil Type C-NiNb₂O₆ (columbite type) and R-NiNb₂O₆ (rutil type) single crystals were prepared by solid state reactions. C-NiNb₂O₆ a = 14.032; b = 5.687; c = 5.033 Å, space group D—Pbcn. R-NiNb₂O₆ a = 4.710; c = 3.038 Å, space group D—P4₂/mnm. The metal positions of the rutil structure are statisticaly occupied by Ni²⁺ and Nb⁵⁺ ions. R-NiNb₂O₆ is in respect to lower temperatures a metastable compound.     

Weitere metastabile Verbindungen mit Tunnelstruktur BaCa2Er10O18 und BaCa2Yb10O18

Single crystals of the unknown compounds BaCa₂Er₁₀O₁₈ (A) and BaCa₂Yb₁₀O₁₈ (B) were prepared by a high-temperature CO₂-laser technique and investigated by X-ray work. (A) and (B) are metastable compounds with an Ln₁₀O₁₈⁶⁻ framework. Two types of tunnels built up by this framework are occupied statistically and in a disordered manner by Ba²⁺, Ca²⁺ and Ln³⁺ ions. The relationship with compounds of the formula AB₂Ln₆O₁₂ are discussed.     

Eu3+ und Eu2+ in Oxometallaten der Zusammensetzung MBeLn2O5: SrBeEu2O5 und EuBeNd2O5

Eu³⁺ and Eu²⁺ in Oxides of the Composition MBeLn₂O₅: SrBeEu₂O₅ and EuBeNd₂O₅ Single crystals of (I): SrBeEu₂O₅ and (II): EuBeNd₂O₅ were prepared by CO₂-LASER (I) in air and plasma torch (II) technique in H₂ atmosphere. X-ray investigations led to orthorhombic symmetry, space group D-Pnma; (I): a = 9.488, b = 7.156, c = 6.495 Å; (II): a = 9.534, b = 7.225, c = 6.544 Å, Z = 4. Sr²⁺ and Eu³⁺ as well as Eu²⁺ and Nd³⁺ are in statistical distribution within a Kagomé framework. Both compounds are discussed with respect to the monoclinic form of MBeLn₂O₅.     

Zur Kenntnis von Ba6La2Co4O15

About Ba₆La₂Co₄O₁₅ Ba₆La₂Co₄O₁₅ were prepared and investigated by X-ray single crystal work. It crystallizes with hexagonal symmetry, space group C–P6₃mc; a = 11.8082; c = 7.0019 Å; Z = 2. Ba²⁺ show face connected BaO₆-octahedra and larger polyhedra of C.N. = 10 and 12. Co³⁺ is surrounded by four and six (tetrahedra, octahedra) oxygen. The Ba²⁺ and La³⁺ ions occupy one point position statistically.     

Zur Kristallchemie der Kupfer-Lanthanoid-Oxowolframate: (I) triklin-α-CuTbW2O8, (II) monoklin-CuInW2O8 und (III) monoklin-CuYW2O8

The Crystal Chemistry of Copper Rare-Earth Oxotungstates: (I): triclinic-α-CuTbW₂O₈, (II): monoclinic-CuInW₂O₈ and (III): monoclinic-CuYW₂O₈ Single crystals of (I), (II) and (III) were prepared by recrystallisation in closed systems and examined by X-ray technique. (I): space group C? P1 , a = 7.3080, b = 7.8945, c = 7.1476 Å, α = 115.23, β = 116.21, γ = 56.98°, Z = 2; (II): space group C? C2/c, a = 9.6576, b = 11.6496, c = 4.9863 Å, β = 91.17°, Z = 4; (III): space group C? P2/n, a = 10.0504, b = 5.8214, c = 5.0224 Å, β = 94.23°, Z = 2. The crystal structures are discussed with respect to calculations of the coulombterms of lattice energy and possible valence states of Cu²⁺ and Mo⁵⁺.     

Ein Wechsel des Strukturtyps in den Oxiden BaCoGd2O5, BaCoDy2O5 und BaCoY2O5

A Change of Structure Type in the Oxides BaCoGd₂O₅, BaCoDy₂O₅, and BaCoY₂O₅ (I) BaCoGd₂O₅, (II) BaCoDy₂O₅, and (III) BaCoY₂O₅ were prepared for the first time and examined by single crystal work. (I) and (II) belong to the BaNiLn₂O₅-type. (I): a = 3.770; b = 5.860; c = 11.620 Å; Z = 2; (II): a = 3.755; b = 5.798; c = 11.514 Å; Z = 2; space group D–Immm. (III) crystallizes in the BaCuLn₂O₅-type, space group D–Pnma, a = 12.287; b = 5.713; c = 7.067 Å; Z = 4. The coordination of Co²⁺ changes from (I, II) to (III) from octahedral to tetragonal pyramidal.     

Über Erdalkalimetalloxoindate. II. Ein neues Calciumindat: Ca3In2O6

A noval Alkaline Earth Metal Oxoindate: Ca₃In₂O₆. The hitherto unknown compound Ca₃In₂O₆ was prepared and investigated by X-ray single crystal methods. Ca₃In₂O₆ is orthorhombic (a = 10.908, b = 16.45, c = 3.228 Å, space group D Pbam) and has a partial statistically distribution of Ca and In. One of the metal positions is occupied only by Ca. The crystal structure of Ca₃In₂O₆ is similar to the CaFe₂O₄-type.     

Über Oxoindate der Alkalimetalle Zur Kenntnis von Rb2In4O7

Oxoindates of Alkali Metals. On Rb₂In₄O₇ The hitherto unknown Rb₂In₄O₇ crystallizes trigonal with a = 5.62₈, c = 7.34₀Å, c/a = 1.30, z = 1 in thespacegroupD–P3 1m. The atomic parameter see text. The structure derives from a cubic closest packing of O²- with In³⁺ in 1/9 of the tetra-hedral and 2/9 of the ovtahedral sites. Rb substituates 2/3 of the O²- ions of each third layer. The MADELUNG Part of Lattice Energy is calculated and discussed.     

Zur Kristallchemie von Ba3In2Zn5O11. Ein tOxoindat/zinkatsol;zinkat mit Zn10O20- und In4O16-Makropolyedern und erstmals O2− in tetraedrischer Koordination durch Zn2+

On the Crystal Structure of Ba₃In₂Zn₅O₁₁. An Oxoindate/zincatesol;zincate with Zn₁₀O₂₀ and In₄O₁₆ Macropolyhedra with Zn²⁺ in Tetrahedral Coordination by O^2? Ba₃In₂Zn₅O₁₁ was prepared for the first time by a flux technique and investigated by single crystal X-ray work. It crystallizes with cubic symmetry, space group T-F4 3m, a = 13.3588 Å, Z = 8. Zn²⁺ show tetrahedral coordination by O^2?, forming Zn₁₀O₂₀ macropolyhedra. In addition the nZn/Osol;O part of the crystal structure is made up of Zn₁₀O₂₀ parts. Edge connection of four InO₆ octahedra results in In₄O₁₆ groups. The crystal structure will be shown and discussed.     

Über die Kristallstruktur von In3Mo11O17 sowie über physikalische Eigenschaften oligomerer Oxomolybdate

On the Crystal Structure of In₃Mo₁₁O₁₇ and the Physical Properties of Oligomeric Oxomolybdates In₃Mo₁₁O₁₇ is characterized by its molybdate framework Mo₂₂O₃₄^8? belonging to the general series Mo_4n+2O_6n+4^x? (with n = 5). The phase grows in star-like aggregates and crystallizes within the orthorhombic system (a = 988.0(2) pm, b = 951.2(2) pm, c = 3 176.7(4) pm). There are oligomeric clusters built from five trans edge-sharing Mo₆ octahedra, surrounded by O atoms over all empty edges according to the Aufbau principle Mo₂₂OOO. In the remaining structural channel one finds an In₆⁸⁺ polycation which is geometrically equivalent with the one of In₁₁Mo₄₀O₆₂. The Mo—O and Mo—Mo distances within the cluster are the same like in In₁₁Mo₄₀O₆₂, too, but there are shorter inter cluster distances (306 pm) in In₃Mo₁₁O₁₇. Disorder in the structure may be understood in terms of the presence of constitutional isomers. While the electrical resistivity of PbMo₅O₈ resembles the one of a strongly disturbed metal (with a local minimum around 120 K), the temperature characteristic of Tl_0.8Sn_0.6Mo₇O₁₁ is typical for a semiconductor. Oxomolybdates with even longer oligomers like In₁₁Mo₄₀O₆₂ and In₃Mo₁₁O₁₇ show metallic conductivity. This course corresponds with the sizes of the clusters and their electronic intercoupling which can be estimated from the specific lengths of the inter cluster distances. The effective magnetic moment grows with increasing cluster length from 0.97 μ_B (PbMo₅O₈) to 1.40 μ_B (In₁₁Mo₄₀O₆₂) per cluster (exception: In₃Mo₁₁O₁₂), and so does the contribution of the temperature-independent paramagnetism (from 890 to 2191 × 10^?6$ \frac{{{\rm emu}}}{{{\rm mol}}} $ per cluster). Thus, a single condensed octahedron carries roughly 440 × 10^?6$ \frac{{{\rm emu}}}{{{\rm mol}}} $ as a temperature-independent paramagnetism, similar to the M₆X₁₇ halide clusters. In₁₁Mo₄₀O₆₂ shows an interesting change in the temperature dependence of its magnetic suszeptibility.     

Ein neuer Strukturtyp zur Formel ABLn2O5 Zur Kenntnis von BaNiNd2O5

A New Crystal Structure of ABLn₂O₅ Compounds. About BaNiNd₂O₅ The compound BaNiNd₂O₅ was prepared by solid state reaction. Single crystal examination show a new structure type (a = 3.829(2), b = 5.932(3), c = 11.649(3) Å space group D–Immm, Z = 2) with Ni²⁺ in octahedral coordination. The surrounding of Ba²⁺ and Nd³⁺ conforms to BaPtNd₂O₅ with significant differences of the polyhedra connection.     

New Pyrochlore Pb[In0.5 Sb1.5]O6.5

From the study of the hypothetical series Pb[PbIn_c–2pSb_c]O_6+p (O ? p < 1; 0 ? c < 2), the existence of the cubic pyrochlore Pb₂^II[In_0.5Sb_1.5]O_6.5 has been established. This compound was obtained as an orange yellow powder, S.G. Fd4 m (No. 227), Z = 8, a = 10.5892(1) Å, V = 1187.38(3) ų, D_c = 8.48 M gm^?3. For Pb in 16(c) positions, In and Sb (1:3) randomly distributed in 16(d), oxygen atoms in 48(f) and in a half of the 8(a) sites, and oxygen positional parameter x = 0.429 (origin at center, 3 m), R = 0.062. The apparent interatomic distances (Å) are determined: Pb? O = 2.612; (In, Sb)? O = 2.019.     

Synthese und Struktur des ersten ternären Blei(II)-Oxocuprats(I): PbCu2O2

Synthesis and Structure of the First Ternary Lead(II) Copper(I) Oxide: PbCu₂O₂ PbCu₂O₂ can be prepared by solid state reaction or by precipitation from a basic aqueous solution. Single crystals of the new compound were prepared by recrystallisation from a molten mixture (PbO? Cu₂O) and investigated by X-ray diffractometer technique. PbCu₂O₂ crystallizes isotypically with the homologue silver compound PbAg₂O₂ (monoclinic with a = 8.22₃ Å, b = 8.28₉ Å, c = 6.01₅ Å, β = 132.6₂°, Z = 4, space group C? C 1 2/c 1). The crystallographic data from the X-ray investigation are reported. The structure is built by endless [PbO_4/4]- and [CuO_2/4]-chains. Pb²⁺ has a one-sided asymmetric coordination with four next oxygen neighbours and Cu⁺ forms a stretched dumbbell with two oxygen atoms.     

Die Photolumineszenz der dreiwertigen Seltenen Erden in den Perowskitstapelvarianten Ba2La2−xSE MgW2□O12, Ba6Y2−xSEW3□O18 und Sr8SrGd2−x SEW4□O24

Photoluminescence of Trivalent Rare Earths in Perovskite Stacking Polytypes Ba₂La_2?x RE MgW₂□O₁₂, Ba₆Y_2?x RE W₃□O₁₈, and Sr₈SrGd_2?xRE W₄□O₂₄ Rhombohedral 12 L stacking polytypes Ba₂La_2?xREMgW₂□O₁₂ show with RE³⁺ = Pr, Sm, Eu, Tb, Dy, Ho, Er, Tm; the 18 L stacking polytypes Ba₆Y_2?xREW₃□O₁₈ and the polymorphic perovskites Sr₈SrGd_2?xREW₄□O₂₄ with RE³⁺ = Sm, Eu, Dy, Ho, Er visible photoluminescence. The concentration dependence and the influence of the coordination number of the rare earth are reported.     

Rb2Co3(H2O)2[B4P6O24(OH)2]: Ein Borophosphat mit ‐Tetraeder‐Anionenteilstruktur und Oktaeder‐Trimeren (CoO12(H2O)2)

Rb₂Co₃(H₂O)₂[B₄P₆O₂₄(OH)₂]: A Borophosphate with ‐Tetrahedral Anionic Partial Structure and Trimers of Octahedra (Co O₁₂(H₂O)₂) Rb₂Co₃(H₂O)₂[B₄P₆O₂₄(OH)₂] is formed under mild hydrothermal conditions (T = 165 °C) from mixtures of RbOH_(aq), CoCl₂, H₃BO₃, and H₃PO₄ (molar ratio 1 : 1 : 1 : 2). The crystal structure (orthorhombic system) was solved by X‐ray single crystal methods (space group Pbca, No. 61; R‐values (all data): R1 = 0.0699, wR2 = 0.0878): a = 950.1(1) pm, b = 1227.2(2) pm, c = 2007.4(2) pm; Z = 4. The anionic partial structure consists of tetrahedral [B₄P₆O₂₄(OH)₂^8–] layers, which contain three‐ and nine‐membered rings. Co^II is octahedrally coordinated by oxygen and oxygen and H₂O ligands, respectively (coordination octahedra CoO₆ and CoO₄(H₂O)₂). Three adjacent coordination octahedra are condensed via common edges to form trimeric units (CoO₁₂(H₂O)₂). The oxidation state +2 of cobalt was confirmed by magnetic measurements. The octahedral trimers are quasi‐isolated. No long‐range magnetic ordering occurs down to 2 K. Rb⁺ is disordered over three crystallographically independent sites within channels of the structure running parallel [010]; the coordination sphere of Rb⁺ is formed by nine oxygen species of the tetrahedral layers, one OH group and one H₂O molecule.     

Zur Polymorphie von In5Br7

On the Polymorphism of In₅Br₇ The existence of two polymorphs of In₅Br₇ has been proved by single crystal structure determinations. In₅Br₇ (tP192) crystallizes with the tetragonal space group P4₁2₁2 and lattice parameters a_t = 1318.9(5) pm and c_t = 3723.8(9) pm (293 K). Concerning monoclinic In₅Br₇ (mC192), the centrosymmetric space group C2/c with lattice parameters a_m = 1867.3(4) pm, b_m=1867.0(5) pm, c_m = 1918.0(7) pm, and β_m = 103.96(2)° (293 K) has been confirmed. Both modifications of In₅Br₇ are built up from layers of the same type. These layers with a thickness of about 930 pm consist of structure fragments [InBr₂]⁴⁺ and [InBr₁₂]^4–. The anion is composed of two ethan‐like [InBr₆]^2– units, which contain In–In bonds. The stacking sequence of the layers with symmetry C 1 2 (1) differs for the two modifications of In₅Br₇. The tetragonal form is generated by applying a 4₁ screw axis; the monoclinic polymorph is formed by introducing inversion centers between the layers. The adequate name of In₅Br₇ = In[InBr₆]Br is triindium(I)‐hexabromodiindate(II)(In–In)‐bromide.