Investigation on the Growth and Properties of Six Garnet Single Crystals with Large Lattice Constants

2021 ◽  
pp. 2000221
Author(s):  
Zhiyuan Han ◽  
Dunlu Sun ◽  
Huili Zhang ◽  
Jianqiao Luo ◽  
Cong Quan ◽  
...  
1996 ◽  
Vol 51 (10) ◽  
pp. 1407-1410 ◽  
Author(s):  
B. Wedel ◽  
Hk. Müller-Buschbaum

Single crystals of Ba2Nb2TeO10) have been prepared by solid state reactions in air. X-ray investigations led to orthorhombic symmetry, space group D152h-Pbca, a = 7.242(4), b = 12.433(3), c = 9.932(3) Å. Z = 4. Nb5+ and Te6+ show octahedral coordination by O2- . The crystal structure is characterized by planes of edge- and corner-sharing NbO6- and TeO6octahedra. It is shown that in spite of nearly identical lattice constants of Ba2Nb2TeO10 with compounds of the composition M0,5BaNbTe2O9 the so far unknown crystals of these substances may not be derived from the Ba2Nb2TeO10 type.


2004 ◽  
Vol 59 (9) ◽  
pp. 985-991 ◽  
Author(s):  
Sabine Strobel ◽  
Thomas Schleid

Quaternary strontium copper(I) lanthanoid(III) selenides are formed by the oxidation of elemental strontium, copper and the corresponding lanthanoid with selenium. Orange to red needle-shaped single crystals of SrCuPrSe3 and SrCuCeSe3 have been synthesized by heating mixtures of Sr, Cu, Pr / Ce and Se with CsI as a flux in evacuated silica tubes to 800°C for 7 d. Both compounds crystallize orthorhombically in space group Pnma with four formula units per unit cell, but with unlike lattice constants (a = 1097.32(6), b = 416.51(2), c = 1349.64(8) pm for SrCuPrSe3 and a = 846.13(5), b = 421.69(2), c = 1663.42(9) pm for SrCuCeSe3) and therefore different structure types. The Pr3+ cations in SrCuPrSe3 are surrounded octahedrally by six Se2− anions forming chains of edge-sharing [PrSe6]9− octahedra that are joined by common vertices. Together with [CuSe4]7− tetrahedra they form [CuPrSe3]2− layers piled up parallel (001). Between those layers the Sr2+ cations are coordinated by seven Se2− anions in the shape of capped trigonal prisms linking the structure in the third dimension. On the other hand in SrCuCeSe3 the Ce3+ cations as well as the Sr2+ cations adopt a coordination number of seven. Since the bonding distances between cerium and selenium match with those of strontium and selenium the two crystallographically independent sites of these cations are occupied statistically by Ce3+ and Sr2+ with equal ratios. Nevertheless, there is a close structural relationship between SrCuPrSe3 and SrCuCeSe3. Similar to SrCuPrSe3 where Cu+ and Pr3+ cations together with Se2− anions form [CuPrSe3]2− layers parallel (001), the Cu+ cations and [(Ce1/Sr1)Se7]11.5− polyhedra in SrCuCeSe3 build strongly puckered layers which are connected by (Ce2)3+/(Sr2)2+ cations. The copper selenium part in both compounds correlates as well, with [CuSe4]7− tetrahedra linked by common vertices to form [CuSe3]5− chains running along [010].


2005 ◽  
Vol 277 (1-4) ◽  
pp. 308-313 ◽  
Author(s):  
R. Almeida Silva ◽  
G. Tirao ◽  
C. Cusatis ◽  
J.P. Andreeta

1978 ◽  
Vol 33 (2) ◽  
pp. 146-148 ◽  
Author(s):  
Hk. Müller-Buschbaum ◽  
M. Harder

Single crystals of the compound Ba2Fe11Al11O34 were prepared by solid state reaction (1700 °C) of BaO-Fe2O3-Al2O3 mixtures. The crystal structure was investigated by X-ray data (space group D46h-P63/mmc, lattice constants: a = 565.3, c = 2281.0 pm). Ba2Fe11Al11O34 is isotypic with Na2O · 11 Al2O3, the structure of β-alumina


1998 ◽  
Vol 194 (2) ◽  
pp. 203-208 ◽  
Author(s):  
Kiyoshi Shimamura ◽  
Vladimir V. Kochurikhin ◽  
Hiroaki Takeda ◽  
Tsuguo Fukuda

2015 ◽  
Vol 15 (7) ◽  
pp. 3131-3136 ◽  
Author(s):  
Yingxin Cui ◽  
Xiaobo Hu ◽  
Kun Yang ◽  
Xianglong Yang ◽  
Xuejian Xie ◽  
...  

1998 ◽  
Vol 53 (3) ◽  
pp. 283-286 ◽  
Author(s):  
L. Wulff ◽  
Hk. Müller-Buschbaum

Abstract Single crystals of the hitherto unknown compound SrMnTeO6 have been prepared from Sr(OH)2 ·8H2O , MnCO3(aq) and TeO2 in air by crystallization below the melt range. X-ray investigations showed hexagonal symmetry, space group D33h -P6̅2m, lattice constants a = 5.143( 1), c = 5.384(2) A, Z = 1. SrMnTeO6 is characterized by staggered [(Mn/Te)6O18] Kagome layers along [001]. These layers are connected by Sr2+ ions, resulting in SrO6 prisms isolated from each other. The structure is discussed with respect to the connection of Kagome nets in the quaternary oxides of the Ba3Ln4O9 type.


1977 ◽  
Vol 32 (6) ◽  
pp. 609-611 ◽  
Author(s):  
H.-R. Freund ◽  
Hk. Müller-Buschbaum

Single crystals of the compound Ho2Cu2O5 were obtained by melting the oxide mixture (2 CuO : 1 Ho2O3), using KF as a flux. The crystal structure was investigated by single crystal X-ray data (Space group C2v9-P 21 nb, lattice constants: a = 1247.8, b = 1081.3, c = 349.5 pm).


1995 ◽  
Vol 50 (8) ◽  
pp. 1167-1170 ◽  
Author(s):  
E. Peters ◽  
Hk. Müller-Buschbaum

Black single crystals of Ti0.33Ta0.67O2 have been prepared by CO2-LASER techniques heating a mixture of TiO and Ta2O5 to T > 2000 °C. The titanium tantalum oxide crystallizes with tetragonal symmetry, space group D144h -P42/mnm, lattice constants a = 4.7344(6) Å c = 3.0504(2) Å, Z = 2. Ti0.33Ta0.67O2 represents the compound TiTa2O6 with rutile structure because of the statistical distribution of Ti2+ and Ta5+. The composition of rutile-type compounds is discussed in more general terms.


2006 ◽  
Vol 3 (8) ◽  
pp. 2665-2668 ◽  
Author(s):  
Duck-Tae Kim ◽  
Sang-An Park ◽  
Woon-Jo Jeong ◽  
Gye-Choon Park ◽  
Moon-Seog Jin ◽  
...  

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