Prototype structure of Pb5Ge3O11

The prototypic structure of the optically active ferroelectric Pb₅Ge₃O₁₁ has been deduced from packing considerations and refined from single-crystal diffractometer data. Interleaving segments of the apatite and nasonite structures in layers perpendicular to c gives the lead germanate structure. The space group of the prototype is $\text{P}\text{6}$, with a = 10.190, c = 10.624 Å, and Z = 3. Atomic coordinates were refined to give an R-factor of 0.093 using 463 X-ray reflections. The structure contains tetrahedral GeO₄ groups and double tetrahedral Ge₂O₇ groups in equal numbers. Lead is found in both trigonal pyramid and trigonal prism configurations.     

Compound formation in the System PbGeO3?Pb5Ge3O11

Compound formation in the system PbGeO₃? Pb₅Ge₃O₁₁ was studied by thermal analysis and high-temperature X-ray diffraction. New modifications of PbGeO₃ and Pb₅Ge₃O₁₁ were prepared by the simultaneous hydrolysis of lead and germanium alkoxides, followed by washing and drying; the former has a hexagonal unit cell with a = 15.573 Å and c = 7.240 Å, and the latter has an orthorhombic crystal structure with a = 5.081 Å, b = 7.301 Å and c = 8.817 Å. They are transformed to the known monoclinic and hexagonal modifications at 575 to 610°C and 410 to 450°C, respectively. No compound of Pb₃Ge₂O₇ was confirmed. The structures of germanate groups in the lead germanate compounds are discussed on the basis of the infrared spectral data.     

Ca7.96Cu0.04Ge5O18: a new calcium germanate with GeO4 and Ge3O10 units

The title compound, octa­calcium copper penta­germanium octa­deca­oxide, represents a new inter­mediate phase between CaO and GeO₂, and has not previously been reported in the literature. The structure consists of three different Ge sites, two of them on general 8d positions, site symmetry 1, one on special position 4d, site symmetry 2. Three of the five Ca sites occur on 8d positions, site symmtery 1, one Ca is on 4b with site symmetry and one Ca is on 4c with site symmetry 2. All nine O atoms have symmetry 1 (8d position). By sharing common edges, the Ca sites form infinite bands parallel to the c axis, and these bands are inter­connected by isolated GeO₄ and Ge₃O₁₀ units. These (100) layers are stacked along a in an ABAB… sequence, with the B layer being inverted and displaced along b/2.     

RADIATION-INDUCED CHANGES IN THE STRUCTURE AND FERROELECTRIC PROPERTIES OF Pb5Ge3O11 SINGLE CRYSTALS

Journal of Structural Chemistry - Perfect stoichiometric Pb5Ge3O11 single crystals are irradiated with 60Co γ-rays (1·106 Rad) and high-energy electrons (0.13 e/cm2, 0.89 e/cm2,...     

Preparation and Optical Properties of Gold-Dispersed BaTiO3, PGO (Pb5Ge3O11) and PLT (Pb1-1.5xLaxTiO3) Thin Films by Sol-Gel Process

Gold-dispersed BaTiO₃, PGO and PLT thin films, which will be used for third-order nonlinear optical devices, were prepared by sol-gel process with spin-coating using HAuCl₄4H₂O, Ba(CH₃COO)₂, Ti[O(CH₂)₃CH₃]₄, Pb(CH₃COO)₂3H₂O, Ge[O-n-C₄H₉]₄, La(CH₃COO)₃1.5 H₂O as starting materials. The thin films were heat-treated in air at temperatures ranging from 400 to 800 for 1 h. The nonlinear optical property of these thin films was measured by the degenerate four-wave mixing (DFWM) method using a frequency-doubled Nd: YAG laser with 20 ps pulse duration. Third-order nonlinear susceptibility χ⁽³⁾ of gold-dispersed BaTiO₃, PGO and PLT thin films with 5 vol% of gold were 1.410⁻⁶ esu, 3.510⁻⁷ esu respectively. The large χ⁽³⁾ may be ascribed to the high dielectric constant of the films.     

On the high-temperature phase transition of Gd5Si2Ge2

The first-order monoclinic-to-orthorhombic (beta-->gamma) phase transition of the giant magnetocaloric material Gd(5)Si(2)Ge(2) was studied using in situ high-temperature single-crystal X-ray diffraction. A special crystal mounting procedure was developed to avoid crystal contamination by oxygen or nitrogen at high temperatures. The elastic beta-->gamma transformation occurs at 300-320 degrees C during heating, and it is reversible during fast and slow heating and slow cooling but irreversible during rapid cooling. Contrary to theoretical predictions, the macroscopic distribution of the Si and Ge atoms remains the same in both the orthorhombic gamma-polymorph and the monoclinic beta-phase. It appears that interstitial impurities may affect stability of both the monoclinic and orthorhombic phases. In the presence of small amounts of air, the beta-->gamma transformation is complete only at 600 degrees C. The interslab voids, which can accommodate impurity atoms, have been located in the structure, and an effect of partially filling these voids with oxygen or nitrogen atoms on the beta-gamma transition is discussed.     

Yb8Ge3Sb5, a metallic mixed-valent Zintl phase containing the polymeric 1 infinity[Ge3 4-] anions

Yb8Ge3Sb5 is a nonclassical Zintl phase with metallic properties arising from the electropositive "spectator" cations of Yb. This compound contains the new Zintl anion 1infinity(Ge3)4- and is stabilized via a combination of Yb2+ and Yb3+ ions.     

Ca3ZnGeO2[Ge4O12]: a Ca–Zn germanate related to the mineral taikanite

The title compound, Ca₃ZnGeO₂[Ge₄O₁₂] (tricalcium zinc germanium dioxide dodecaoxidotetragermanate), adopts a taikanite‐type structure. The tetrahedral [Ge₄O₁₂] chain geometry is very similar to that of the silicate chain of taikanite, i.e. BaSr₂Mn³⁺₂O₂[Si₄O₁₂], while the major difference is found parallel to the c axis. In taikanite, Mn³⁺ octahedra form an infinite zigzag chain, whereas the title compound has a chain of distorted ZnO₆ octahedra, which alternates with distorted GeO₄ tetrahedra connected to each other via two common edges. Eightfold‐coordinated Ca²⁺ polyhedra and ZnO₆ octahedra form a slab parallel to (001) which alternates with another slab containing the tetrahedrally coordinated Ge sites along the c axis.     

Cluster self-organization of silicate and germanate systems: Suprapolyhedral precursor nanoclusters and self-assembly of tetrahedral structures of the family A2T2O5 (A = Li, Na; T = Si, Ge): Li2T2O5, Li4Ge3SiO10, Li2Si2O5, and A2Si2O5

Modeling of atomic species (An clusters in the form of atoms or Kn polyhedra, where n is the number of atoms or polyhedra) corresponding to the initial stage of evolution of a chemical system has been carried out. Three series of K4 clusters built of different T tetrahedra (L and T) have been recognized. For L₂T₂ clusters, six geometrically and symmetrically different types of suprapolyhedral clusters have been discovered. The model has been used to identify precursor clusters in A₂T₂O₅ (A = Li, Na; T = Si, Ge) framework structures: A-type Li₂T₂O₅ with space group Cc, B-type Li₄Ge₃SiO₁₀ with space group Abm2, C-type Li₂Si₂O₅ with space group Ccc2, and D-type A₂Si₂O₅ with space group Pbcn. Three (of the six possible) types of suprapolyhedral precursor nanoclusters K4 in the four structures have been identified. The full 3D reconstruction of the self-assembly scenario of crystal structures is as follows: precursor nanocluster ?? primary chain ?? microlayer ?? microframework ?? ?? framework. The bifurcation of structural evolution pathways (structural branching points) at the suprapolyhedral level for type A and B structures is found to occur only when a microframework is formed of equivalent microlayers.     

Die Substituierbarkeit von Blei in Pb3Ge2O7 durch Cd,Sr und Ba

Up to 25% of the lead atoms can be substituted by Sr in Pb₃Ge₂O₇ without change in structure. The existence of Pb₈Cd(Ge₂O₇)₃ with the structure of barysilit has been confirmed in accordance with the literature. A new phase with barysilitstructure was observed in the system BaO/PbO/GeO₂.

     

Synthesis, structure, and bonding of the nonclassical Zintl phase K5As3Pb3

The title phase was synthesized by direct fusion of a stoichiometric amount of the elements followed by annealing at 650 degrees C for 3 weeks. The compound crystallizes in the orthorhombic space group Pnma (No. 62), Z = 4, with a = 19.451(6) A, b = 12.164(3) A, c = 6.581(1) A. The compound is made up of As(3)Pb(3)(5-) crown clusters that can be likened geometrically and electronically to 6-atom hypho-clusters derived from a tricapped trigonal prismatic closo parent. These crowns are interconnected via intercluster Pb-Pb bonds to form infinite chains along the b axis, which means the compound contains an extra two cations and two electrons per formula unit. Extended Hückel calculations indicate that the two additional electrons per cluster are accommodated in pi states on the cluster and predict that the phase should be semiconducting. The latter is confirmed by microwave resistivity measurements, rho(298) = 1.0 x 10(2) microOmega.cm; (deltarho/deltaT)/rho = -0.14(3) K(-)(1).     

Thermogravimetric studies of the decomposition of red lead (Pb3O4)

TG measurements have been performed on red lead under (a) isothermal (b) dynamic conditions, under a constant flow of nitrogen.The results have been analyzed to establish the decomposition kinetics and calculate the activation energies.In the case of isothermal decomposition, it is concluded that rate of diffusion of gaseous products is the controlling factor, while in dynamic decomposition nucleation and growth within the Pb₃O₄ particles is important.

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Zusammenfassung TG-Messungen wurden an Zinoberrot unter a) isothermen und b) dynamischen Bedingungen, in einem konstanten Stickstoffstrom durchgeführt. Die Ergebnisse wurden analysiert um die Zersetzungskinetik zu ermitteln und die Aktivierungsenergien zu berechnen. Im Falle der isothermen Zersetzung wurde gefolgert, da\ die Diffusionsgeschwindigkeit der gasförmigen Produkte der steuernde Faktor ist, wÄhrend bei der dynamischen Zersetzung die Keimbildung und das Wachstum innerhalb der Pb₃O₄-Teilchen von Bedeutung ist.

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Résumé On a effectué des mesures TG sur du cinabre en conditions a) isothermes et b) dynamiques, sous courant constant d'azote. On a analysé les résultats afin d'établir la cinétique de la décomposition et de calculer les énergies d'activation. Dans le cas de la décomposition isotherme, on a conclu que la vitesse de la diffusion des produits gazeux était le facteur contrÔlant la réaction, tandis que lors de la décomposition dynamique la nucléation et la croissance des particules de Pb₃O₄ jouaient un rÔle important.

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. . , . Pb₃O₄.

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The authors thank Nobel's Explosives Co. Ltd. for financial support and supply of materials, and Science Research Council for granting a Co-operating Award in Science and Engineering (CASE) research studentship to one of us (S. S. Al-Kazraji).     

Synthesis, structural characterization, and thermal stability of a new layered germanate structure, Na4Ge16O28(OH)12

The new layered germanate structure Na4Ge16O28(OH)12 has been synthesized under hydrothermal conditions and characterized by single-crystal X-ray diffraction, FTIR, and SEM. The crystal lattice parameters are a = 7.3216(6) A, b = 14.3986(9) A, c = 7.7437(6) A, alpha = 90.0 degrees, beta = 100.179(7) degrees, gamma = 90.0 degrees, and V = 803.5(1) A3. The space group is C2/m with Z = 1. The germanium oxide sheets are connected non-covalently via electrostatic interactions with the sodium cations and H-bridging. At temperatures above 400 degrees C, the structure starts decomposing into sodium enneagermanate (Na4Ge9O20), germanium dioxide, and water as determined by powder X-ray diffraction, TGA, DTA, DSC, and GCMS.     

Refined crystal structures of the scandium garnets Ca3Sc2Si3O12, Ca3Sc2Ge3O12, and Cd3Sc2Ge3O12

Journal of Structural Chemistry -     

Struktur‐Eigenschafts‐Beziehung von Cu5Pb6O3Cl11, einer gut Kupferionen leitenden Verbindung

Structure‐Behaviour‐Relation of Cu₅Pb₆O₃Cl₁₁, a Good Solid State Ionic Conductor for Cu⁺‐Ions A new compound within the group of coin metal lead(II) oxide halides is found and characterized by X‐ray single crystal structure determination in a temperature range from 120 K to 400 K. Cu₅Pb₆O₃Cl₁₁ shows a new crystal type structure with a = 21.098(4) Å, b = 10.233(2) Å, c = 12.224(2) Å, β = 124.08(3)°, Z = 4 and space group C 2/c (No. 15) at 120 K. There are found isolated oxidic chains built of OPb₄ tetrahedra beside columnar areas consisting of CuCl. In this halidic partial structure are a lot of empty and partially occupied Cl₄‐tetrahedra. This structural characteristic seems to be source of a very good conductivity of copper ions, like in microscopic and nanoscaled composites of Al₂O₃ and AgI.