Ba8Cu16P30 – eine neue ternäre Variante des Clathrat I-Strukturtyps

Ba₈Cu₁₆P₃₀ – a New Ternary Variant of the Clathrate I Type Structure Ba₈Cu₁₆P₃₀ (a = 14.117(1) Å, b = 10.093(1) Å, c = 28.022(2) Å) was prepared by heating a mixture of the elements (800°C; excess of Ba and P; removal of the by-products by acetic acid/H₂O₂). The compound crystallizes orthorhombically (Pbcn; Z = 4) in a new superstructure of the cubic clathrate I type structure with an ordered distribution of the atoms. The structure is characterized by a three-dimensional framework of CuP₄ tetrahedra with cavities in the form of pentagonal dodecahedra and tetrakaidecahedra, which are occupied by the Ba atoms. The compound shows semiconduction, therefore the composition should be Ba₈Cu_15.5P_30.5.     

Order and disorder in Ca2ND0.90H0.10-A structural and thermal study

The structure of calcium nitride hydride and its deuterided form has been re-examined at room temperature and studied at high temperature using neutron powder diffraction and thermal analysis. When synthesised at 600 °C, a mixture of both ordered and disordered Ca₂ND_0.90H_0.10 phases results. The disordered phase is the minor component and has a primitive rocksalt structure (spacegroup Fm3m) with no ordering of D/N on the anion sites and the ordered phase is best described using the rhombohedral spacegroup R-3m with D and N arranged in alternate layers in (111) planes. This mixture of ordered and disordered phases exists up to 580 °C, at which the loss of deuterium yields Ca₂ND_0.85 with the disappearance of the disordered phase. In the new ordered phase there exists a similar content of vacancies on both anion sites; to achieve this balance, a little N transfers onto the D site, whereas there is no indication of D transferring onto the N-sites. These observations are thought to indicate that the D/N ordering is difficult to achieve with fully occupied anion sites. It has previously been reported that Ca₂ND has an ordered cubic cell with alternating D and N sites in the [100] directions [1]; however, for the samples studied herein, there were clearly two coexisting phases with apparent broadening/splitting of the primitive peaks but not for the ordered peaks. The rhombohedral phase was in fact metrically cubic; however, all the observed peaks were consistent with the rhombohedral unit cell with no peaks requiring the larger ordered cubic unit cell to be utilised. Furthermore this rhombohedral cell displays the same form of N-D ordering as the Sr and Ba analogues, which are metrically rhombohedral.     

The structure of the compound Cd3P2

Structure of Cd₃P₂ (P4₂/nmc, a = b = 8.7390 Å, c = 12.2523 Å) has been solved and refined up to R = 3.78% using precision X-ray diffraction experimental data (λ-MoK _α, graphite monochromator on a primary beam, 11529 reflections). Interatomic distances and valence angles are determined. Phosphorus forms a face-centered cubic lattice in which 3/4 tetrahedral voids are occupied by cadmium atoms in the crystal structure. The structure can be described by two equivalent models in which the positions of cadmium atoms, which occupy tetrahedral voids following the “diamond principle,” are preserved, while the remaining free and occupied voids change their places.     

Reactions of TiCl4 and ZrCl4 with IOCN

On Hexagonal Perovskites with Cationic Vacancies. V. Structure Determination on H? Ba₂Lu_2/3 □ _1/3WO₆ — a Novel Rhombohedral Stacking Polytype with 18 Layers Compounds of type Ba₂B□_1/3W^VIO₆ with B^III ? Gd—Lu, Y are polymorphic They crystallize in a cubic 1:1 ordered perovskite structure and in a new rhombohedral perovskite stacking polytype of 18 L respectively. By intensity calculations out of the three possible stacking sequences (4)(2), (5)(1) and (3)1(1)1 (all space group R3 m) the sequence (5)(1) can be selected. For H? Ba₂Lu_2/3□_1/3WO₆ the refined R′ factor is 14.1%. The structure contains groups of three octahedra connected with another by common faces which are linked with each other by three corner sharing octahedra. In the block of three face sharing octahedra the central octahedral lattice site is vacant, the two outer positions are occupied by tungsten atoms. According to this distribution a direct contact of occupied face sharing octahedra is absent.     

Hochdrucksynthese und Kristallstruktur von YbH2, 67

High Pressure Synthesis and Crystal Structure of YbH_2.67 Ytterbiumhydrides can be synthesized by reaction of ytterbium metal in hydrogen atmosphere above 600 K. The experiments were carried out in the pressure range from 200 to 3200 bar. X‐ray investigations on powdered samples and elastic neutron diffraction experiments on deuterated compounds led to a complete structure determination. YbH_2.67 is obtained at reaction pressures of 200, 1400 und 3200 bar. In contrast to reports in literature the deuterides crystallize with trigonal symmetry (P3¯1m, a = 6.344(1)Å, c = 9.002(1)Å, Z = 9) and not in the cubic crystal system. The composition YbD_2.67 was additionally checked by chemical analysis. The crystal structure can be described as a close packing of ytterbium atoms (stacking sequence …ABC…) in which all tetrahedral holes and 2/3 of the octahedral holes are occupied in an ordered manner by hydrogen. Magnetic susceptibility measurements are in agreement with literature data.     

Struktur und Eigenschaften quaternärer Chalkogenide MIAIIIBIVX. III. Über die Verbindungen AgTiZrTe4 und Ag2TiZrTe4

Structure and Properties of Quaternary Chalcogenides M^IA^IIIB^IVX . III. On the Compounds AgTiZrTe₄ and Ag₂TiZrTe₄ Preparation and properties of the compounds AgTiZrTe₄ and Ag₂TiZrTe₄ are reported. The structure deduced from X-ray diffraction diagrams is closely related to the structure of TiZrTe₄ showing an ordered accomodation of Ti and Zr atoms at the octahedral sites of the CdI₂ type structure. The interlayers free of Ti and Zr atoms are suggested to be in part occupied by Ag⁺ ions in an ordered sequency, which allows to explain the occurrence of 8 Te layers in the repeating unit.     

Cation ordering in Ca2La8(SiO4)6O2

The distribution of La³⁺ and Ca²⁺ over the cation sites in Ca₂La₈(SiO₄)₆O₂ was determined by single-crystal X-ray diffraction. Ca₂La₈(SiO₄)₆O₂ has the apatite structure, and all available evidence indicates that the space group is $\text{P6}{}_3\text{m}$, thus precluding a completely ordered structure. The 6h lattice sites are occupied by La³⁺. In contrast, the 4f sites are occupied equally by La³⁺ and Ca²⁺ ions. Consideration of the properties of the La³⁺ and Ca²⁺ ions suggests that this distribution is thermodynamically favored for this composition. A simple Ising model suggests ordered columns. These would not be precluded by space group $\text{P6}{}_3\text{m}$, if the correlation between adjacent columns were random.     

Synthesis and Characterization of Copper Hexathiometadiphosphate Cu2P2S6

Copper hexathiometadiphosphate, Cu₂P₂S₆, was synthesized and characterized. Brick‐red copper hexathiometadiphosphate Cu₂P₂S₆ crystallizes in the tetragonal space group P4₂/mnm (no. 136) with a = b = 5.2565(7), c = 15.066(3) Å and V = 416.3(1) ų in a novel structure type. This is the first hexathiometadiphosphate, whose crystal structure is based on a slightly distorted cubic closest packing of sulfur atoms. 1/3 of the tetrahedral voids are occupied by Cu and P in an ordered fashion, thus resulting in a layered structure. The structural motif of layers composed of corner‐sharing CuS₄ tetrahedra (comparable to red HgI₂) that are separated by [P₂S₆]^2– anions orientated perpendicular to these layers, is rarely found in solid state chemistry. The compound is diamagnetic and shows negligible electronic conductivity. Electronic structure calculations and UV/Vis measurements point to a bandgap in the visible range and explain the red color of the compound. Additionally, the oxidation state +1 for Cu was confirmed by the electronic structure calculations. The thermal properties of Cu₂P₂S₆ were investigated by DTA.     

Cyclische Phosphidostannat(III)-Anionen [Sn12P24]36– in Sr3[Sn2P4]

Cyclic Phosphidostannate(III) Anions [Sn₁₂P₂₄]^36– in Sr₃[Sn₂P₄] The metallic lustrous, air sensitive compound Sr₃[Sn₂P₄] was prepared from melts of mixtures of the elements. Sr₃[Sn₂P₄] crystallizes in the orthorhombic system, space group Cmca (a = 2510,4(9), b = 1259,3(6), c = 1869,3(8), Z = 24). In the anionic partial structure six moieties [Sn₂P₆] isostructural to Si₂Cl₆ are linked by each four common P-ligands forming cyclic units [Sn₁₂P₂₄]^36–. The strontium cations are octahedrally coordinated by P. The arrangement can be described as a distorted cubic close packing of P^3– in which in an ordered manner ³/₄ of the octahedral vacancies are occupied by Sr²⁺ and ¹/₄ by Sn₂-dumbbells.     

Synthesis,Single Crystal Growth and Crystal Structure of Ta7Cu10Ga34 – a 8 × 4 × 2 Super Structure of CsCl

Single crystals of Ta₇Cu₁₀Ga₃₄ were grown from the elements in a Cu/Ga melt. Ta₇Cu₁₀Ga₃₄ represents the first ternary compound of the system Ta/Cu/Ga. The crystal structure (Cmmm, oC102, Z = 2, a = 23.803(1), b = 12.2087(4), c = 5.7487(2) Å, 1291 refl. 78 parameters, R₁ = 0.037, wR₂ = 0.070). The crystal structure is characterized by rods of pentagonal prisms MGa₁₀, which are alternatingly occupied by Ta and Cu. Four of these rods are connected to columns running in direction (001). These columns are linked by cubic units TaGa₈, CuGa₈, and GaGa₈. According to the characteristic structural elements and the size of the unit cell Ta₇Cu₁₀Ga₃₄ represents a 8 × 4 × 2 super structure of CsCl or bcc. With respect to the underlying CsCl structure the formula can be written as [Ta₇Cu₁₀Ga₂□₁₃]Ga₃₂, i.e. a cubic primitive packing of 32 Ga atoms with Ta, Cu, and Ga in cubic voids and 13 vacancies. The pentagonal‐prismatic coordination of Ta and Cu can formally be obtained from the cubic primitive packing of Ga atoms by a 45° rotation of a part of the Ga₈ cubes. There is a close similarity to the binary compounds Ta₈Ga₄₁ and Ta_2–xGa_5+x. The first one is also related to a CsCl‐like structure, the latter one contains rods of pentagonal prisms, which form the same columns. There are also relations to the ternaries V₂Cu₃Ga₈ and V₁₁Cu₉Ga₄₆, whose cubic structures are more or less complex variants of CsCl.     

Infinite Gold Zig‐Zag Chains as Structural Motif in Ca3Au3In – A Ternary Ordered Variant of the Ni4B3 Type

New auride Ca₃Au₃In was synthesized from the elements in a sealed tantalum tube in a high‐frequency furnace. Ca₃Au₃In was investigated by X‐ray powder and single crystal diffraction: ordered Ni₄B₃ type, Pnma, a = 1664.1(6), b = 457.3(2), c = 895.0(3) pm, wR2 = 0.0488, 1361 F² values, and 44 variables. The three crystallographically independent boron positions of the Ni₄B₃ type are occupied by the gold atoms, while the four nickel sites are occupied by calcium and indium in an ordered manner. All gold atoms have trigonal prismatic coordination, i.e. Ca₆ prisms for Au1 and Au2 and Ca₄In₂ prisms for Au3. While the Au3 atoms are isolated, we observe Au1–Au1 and Au2–Au2 zig‐zag chains at Au–Au distances of 292 and 284 pm. These slabs resemble the CrB type structure of CaAu. Consequently Ca₃Au₃In can be considered as a ternary auride. Together the Au2, Au3 and indium atoms build up a three‐dimensional [Au₂In] polyanionic network (281–293 pm Au–In) in which the chains of Au1 centered trigonal prisms are embedded. The crystal chemical similarities with the structures of Ni₄B₃, CaAuIn, and CaAu are discussed.     

Zur Struktursystematik der Li2O-Varianten vom Typ Li5MIIIO4

The possibilities to form corresponding to Li₅□₂M^IIIO₄ ordered derivatives of the Li₂O structure using a cubic super cell with a ≈ 2 · a are systematically discussed within some limits (see text ). It is shown that besides of the known examples new ones are to be expected.     

Partial Sn‐atom ordering in Sm3Ga0.80–2.48Sn4.20–2.52

Trisamarium digallide tristannide crystallizes with a partially ordered Pu₃Pd₅‐type structure in space group Cmcm. In a single crystal of Sm₃Ga_1.89(4)Sn_3.11(4), the 8g position is mostly occupied by Sn atoms (93% Sn and 7% Ga), while the 4c and 8f positions are occupied by a Ga/Sn statistical mixture. The evolution of the structure as a function of the Ga content has been studied by X‐ray powder diffraction on ten Sm₃Ga_5−xSn_x samples. It is shown that the 8g position remains occupied essentially exclusively by Sn atoms within the whole homogeneity range, with x ranging from 2.52 to 4.20.     

Phase Transition of a Structure II Cubic Clathrate Hydrate to a Tetragonal Form

The crystal structure and phase transition of cubic structure II (sII) binary clathrate hydrates of methane (CH₄) and propanol are reported from powder X‐ray diffraction measurements. The deformation of host water cages at the cubic–tetragonal phase transition of 2‐propanol+CH₄ hydrate, but not 1‐propanol+CH₄ hydrate, was observed below about 110 K. It is shown that the deformation of the host water cages of 2‐propanol+CH₄ hydrate can be explained by the restriction of the motion of 2‐propanol within the 5¹²6⁴ host water cages. This result provides a low‐temperature structure due to a temperature‐induced symmetry‐lowering transition of clathrate hydrate. This is the first example of a cubic structure of the common clathrate hydrate families at a fixed composition.     

ACu9X4 ‐ Neue Verbindungen mit der CeNi8, 5Si4, 5‐Struktur (A: Sr,Ba; X: Si,Ge)

ACu₉X₄ ‐ New Compounds with CeNi_{8, 5}Si_{4, 5} Structure (A: Sr, Ba; X: Si, Ge) The new compounds SrCu₉Si₄ (a = 8.146(1), c = 11.629(2)Å), BaCu₉Si₄ (a = 8.198(2), c = 11.735(2)Å), SrCu₉Ge₄ (a = 8.273(2), c = 11.909(5)Å), and BaCu₉Ge₄ (a = 8.338(4), c = 12.011(7)Å) are formed by reaction of the elements at 1000° ‐ 1100 °C. They are isotypic (I4/mcm, Z = 4) and crystallize in an ordered variant of the cubic NaZn₁₃ type structure, also built up by the binary phase BaCu₁₃. In the ternary compounds the positions of Cu2 are orderly occupied by copper and silicon and germanium, respectively. This results in a lowering of symmetry and a distortion of the polyhedra. The metallic conductivity of the compounds was confirmed by measurements on BaCu₉Si₄.     

X-ray and neutron powder diffraction study of the double perovskites Ba2LnSbO6 (Ln=La, Pr, Nd and Sm)

The crystal structures of Ba₂LnSbO₆ (Ln=La, Pr, Nd and Sm) at room temperature have been investigated by profile analysis of the Rietveld method using either combined X-ray and neutron powder diffraction data or X-ray powder diffraction data. It has been shown that the structure of Ba₂LnSbO₆ with Ln =La, Pr and Nd are neither monoclinic nor cubic as were previously reported. They are rhombohedral with the space group . The distortion from cubic symmetry is due to the rotation of the LnO₆/SbO₆ octahedra about the primitive cubic [111]_p-axis. On the other hand, the structure of Ba₂SmSbO₆ is found to be cubic. All compounds contain an ordered arrangement of LnO₆ and SbO₆ octahedra.     

High pressure synthesis and crystal structure of NaMn7O12

A new compound, NaMn₇O₁₂, with the perovskite-like arrangement has been synthesized at 80 kbar and 1000°C. This compound is cubic, a = 7.3036 Å, space group Im3 with four formula weights per unit cell. The structure has been solved by Patterson and Fourier synthesis and refined by least-squares based on 142 reflections. The final R and wR factors were 0.025 and 0.033, respectively. The A sites of the perovskite structure are occupied by sodium and manganese atoms in an ordered fashion. The sodium atoms are each surrounded by a 12-oxygen polyhedron whereas the manganese atoms have four nearest oxygens at 1.909 Å forming a square and four more at 2.688 Å forming a rectangle perpendicular to the square. The distortion of the oxygen network from the ideal perovskite structure is similar to that found for In(OH)₃ and Sc(OH)₃.     

Schichtenweise Substitution von Kationen im Lithiumamid: Kaliumtrilithiumamid,KLi3(NH2)4 und Kaliumheptalithiumamid,KLi7(NH2)8

Substitution in Layers of Cations in Lithium Amide: Potassium Trilithium Amide, KLi₃(NH₂)₄, and Potassium Heptalithium Amide, KLi₇(NH₂)₈ Four ternary amides were characterized in the system KNH₂/LiNH₂ by x-ray techniques: K₂Li(NH₂)₃ (dimorphous), KLi(NH₂)₂, KLi₃(NH₂)₄, and KLi₇(NH₂)₈. The compounds were prepared by the reaction of ammonia with the metals in high-pressure autoclaves. The atomic arrangements of the potassium-poor amides, KLi₃(NH₂)₄, and KLi₇(NH₂)₈ which have been investigated by x-ray single crystal analysis are discussed: Layers of edge sharing aniontetrahedra occupied to three quarters by lithium are the dominating structural feature. These layers ? [Li₃(NH₂)₄^?] — are primitively stacked in such a manner that potassium occupies quadratic prismatic sites. In KLi₇(NH₂)₈ the layers are connected alternatively by lithium in tetrahedral sites and potassium in an eightfold coordination. The ordered distribution of the cations is controlled by the orientation of amide ions. KLi₃(NH₂)₄ can structure-geometricly be considered as a further example of an “ordered defect structure” of the ThCr₂Si₂ type structure.     

Controllable synthesis of highly crystallized mesoporous TiO_2/WO_3 heterojunctions for acetone gas sensing

Mesoporous semiconducting metal oxides(SMOs) heterojunctions are appealing sensors for gas detecting.However,due to the different hydrolysis and condensation mechanism of every metal precursor and the contradiction between high crystallinity and high surface area,the synthesis of mesoporous SMOs heterojunctions with highly o rdered mesostructures,highly crystallized frameworks,and high surface area remains a huge challenge.In this work,we develop a novel "acid-base pair"adjusted solvent evaporation induced self-assembly(EISA) strategy to prepare highly crystallized ordered mesoporous TiO_2/WO_3(OM-TiO_2/WO_3) heterojunctions.The WCl_6 and titanium isopropoxide(TIPO) are used as the precursors,respectively,which function as the "acid-base pair",enabling the coassembly with the structure directing agent(PEO-b-PS) into highly ordered meso structures.In addition,PEO-b-PS can be converted to rigid carbon which can protect the meso structures from collapse during the crystallization process.The resultant OM-TiO_2/WO_3 heterojunctions possess primitive cubic mesostructures,large pore size(～21.1 nm),highly crystalline frameworks and surface area(～98 m~2/g).As a sensor for acetone,the obtained OM-TiO_2/WO_3 show excellent re sponse/recovery perfo rmance(3 s/5 s),good linear dependence,repeatability,selectivity,and long-term stability(35 days).     

Pr30Ti24I8O25Se58: Eine hochsymmetrische Struktur mit isolierten [Ti6(O)Se8]‐Clustereinheiten

Pr₃₀Ti₂₄I₈O₂₅Se₅₈: A Highly Symmetric Structure with Isolated [Ti₆(O)Se₈]‐Cluster Units Black crystals of Pr₃₀Ti₂₄I₈O₂₅Se₅₈ have been prepared by the reaction of Pr₂Se₃, Pr₂O₂Se, TiSe_2–x, and I₂ at 900 °C. Its crystal structure can be described as a variation of the NaCl structure type (space group Fm 3 m, a = 2319.91(15) pm, Z = 4). The compound contains the first example of a [Ti₆(O)Se₈] cluster. These clusters form a cubic close packing, where the octahedral and tetrahedral holes are occupied by “superoctahedral” and “supertetrahedral” building units, respectively.