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1.
On the System Ba2Sm 0.67U1?xWxO6 The ordered perovskites Ba2Sm0.67UO6 and Ba2Sm0.67 WO6 are forming a complete serie of solid solutions with 4 formula units Ba2Sm0.67U1?xWxO6 in the unit cell. By diffuse reflectance and i.r.-spectroscopic measurements the relations between color and constitution are shown.  相似文献   

2.
On Hexagonal Perovskites with Cationic Vacancies. XXXIII. Compounds of Type Ba6?xSrxB2?y3+SEy3+W3□O18 In the series Ba6?xSrxLu2?ySEy3+W3□O18 a substitution of Sr2+ for Ba2+ is possible. According to intensity calculations on powder data of BaSr5Lu1,6Ho0,4W3□O18 the compounds crystallize in a rhombohedral 18 L type with the sequence (hhcccc)3; space group R3 m. The refined, intensity related R' value is 11.5%. The differences in properties (diffuse reflectance spectra, photoluminescence) between the hexagonal modifications Ba6B2?y3+SEy3+W3□O18 (B3+ ? Gd, Y, Lu; SE3+ ? Sm, Eu, Tb, Dy, Ho, Er, Tm) and the corresponding cubic HT modifications are discussed.  相似文献   

3.
On Hexagonal Perovskites with Cationic Vacancies. III. Structure Determination on Compounds of Type Ba2B □2/3 ReVIIO6 Compounds of Type Ba2B □2/3 ReVIIO6 with BIII = rare earth, Y. Sc, In belong to the group of hexagonal perovskite stacking polytypes. For BIII = Gd, Y structure determinations with powder data have been performed. The refined R′ factors are 9.11% for Ba2Gd1/3□2/3ReO6 and 12.07% for Ba2Y1/3□2/3ReO6. The structure represents a rhombohedral 12 L type (space group R3 m) with the sequence hhcchhcchhcc. The lattice contains groups of three octahedra connected by common faces which are linked together by a single octahedron via common vertices. In the block of three face-sharing octahedra the central octahedral lattice site is vacant and the two outer positions are occupied by the rhenium atoms. According to this distribution direct contact of occupied face-sharing octahedra is absent.  相似文献   

4.
On Perovskite Phases of the System Ba2Y0,67U1?xWxO6 A solid solution series is formed between the polymorphic perovskites Ba2Y0.67UO6 and Ba2Y0.67WO6 (cubic: a = 8.372 Å; hexagonal: a = 4× 5.881 Å and c = 4× 7.778 Å). The structure is cubic between x = 0.1 and 0.99 and for x > 0.95 hexagonal as well. Strong deviations from the ideal behaviour are detectabel with spectroscopic methods. The shape of the UO6 and WO6 octahedrons experiences only minor changes within the series.  相似文献   

5.
On Hexagonal Perovskites with Cationic Vacancies. XII. Structure Determination on Ba6W42O18 The stacking polytype Ba6W42O18 is the first oxidic variant of the Cs3Tl2Cl9-type. The structure determination gave for the space group R3 c with the sequence (h)6, Z = 3, the refined, intensity related R′ value of 6.8%. The octahedral net consists of groups of two face sharing WO6 octahedra (W2O6/2;O6), which are in the (110) plane displaced against each other. In the doublé octahedra the tungsten atoms are shifted away from their ideal central position (W–W: 2.327 Å) with the result, that the W–W distance has increased to 2.905 Å.  相似文献   

6.
On Hexagonal Perovskites with Cationic Vacancies. XV. Ba9Nb6W□2O27 – the First Perovskite Stacking Polytype of Rhombohedral 27 L-Type The perovskite stacking polytype Ba9NbWVI2O27(white) is the first representative of a rhombohedral 27 L-type. The lattice parameters (trigonal setting) are: a = 5.793 Å; c = 63.41 Å; Z = 3 (?exp = 6.46 g/cm3; ?calc = 6.512 g/cm3). The corresponding TaV -compound is isotypic; it tends to develop stacking faults.  相似文献   

7.
On Hexagonal Perovskites with Cationic Vacancies. XXVIII. Structure of Rhombohedral 9 L Stacking Polytypes Ba3W Nb □O9?x/2x/2 According to the intensity calculations for Ba3W4/3Nb2/3□O26/31/3 and Ba3Nb2□O8□(II) these rhombohedral 9 L compounds crystallize in the space group R3m, sequence (hhc)3. The refined, intensity related R′ values are 6.9% (Ba3W4/3Nb2/3□O26/31/3) and 7.2% (Ba3Nb2□O8□(II)). The relations between the rhombohedral 9 L structure (A3M2□O9) and the palmierite type (A3M2□O8□) are discussed.  相似文献   

8.
On Hexagonal Perovskites with Cationic Vacancies. I. Compounds of the Type Ba2B □2/3ReVIIO6 Compounds of Type Ba2B□2/3ReVIIO6 are formed with BIII = Sm? Gd Ho? Lu, Y, Sc, In (yellow); Tb (black-brown); Dy (yellow-orange). They crystallize with BIII = Sm? Lu, Y and Sc in a rhombohedral layer structure of 12 L-type (space group R3 m; sequence: cchhcchhcchh) with 6 formula units in the unit cell.  相似文献   

9.
On Perovskites Ba2B B TeVIO6 Compounds of composition Ba2BBTeVIO6 with BI = Li, Na; BIII = La, Pr, Nd, Sm, Eu, Gd, Tb, Ho, Yb, Y, In, Sc crystallize in a cubic 1:1 ordered perovskite structure. The vibrational spectroscopic investigations show, that more species of TeO6 octahedra are present in the lattice.  相似文献   

10.
On Hexagonal Perovskites with Cationic Vacancies. XX. Ba6Nb4Zr□o18 - a New Stacking Polytype with a Rhombohedra1 18 L Structure The white Ba6Nb4Zr□O18 crystallizes in a rhombohedral 18 L structure (a = 5.821 Å; c = 42.63 Å; space group R3 m) with three formula units for the trigonal setting (?exp = 6.05 g/cm3; ?calc = 6.271 g/cm3). The corresponding TiIV and HfIV compounds, Ba6Nb4Zr□O18 and Ba6Nb4Hf□O18, are isotypic.  相似文献   

11.
On Hexagonal Perovskites with Cationic Vacancies. XXXII. Photoluminescence of Trivalent Rare Earth in the Systems Ba2?ySryLa2?xRExMgW2□O12 In the series Ba2?ySryLa2?xRExMgW2□O12 the Ba2+ can be completely substituted by Sr2+. All compounds crystallize in the rhombohedral 12 L-type (space group R3 m; sequence (hhcc)3). By doping the stacking polytypes with some of the trivalent rare earths efficient visible photoluminescence is obtained. The simultaneous incorporation of two different rare earth ions leads to two-color-phosphors, which, according to the excitation energy used, emit either mainly the typical spectrum from one or the other activator; the corresponding luminescence mechanism are discussed.  相似文献   

12.
On Hexagonal Perovskites with Cationic Vacancies. XI. Stacking Polytype Ba6W42O18 The white Ba6W42O18, with a cation/vacancy ratio of 2:1 for the octahedral holes, is the first representative of a new stacking polytype for this formula type. It crystallizes in a rhombohedral six layer-structure with ahex = 10.130 Å chex = 13.960 Å Z = 3 (ρexp = 7.38 g/cm3; ρcalc = 7.418 g/cm3).  相似文献   

13.
On Hexagonal Perovskites with Cationic Vacancies. XXIV. Rhombohedral 9 L Stacking Polytypes in the Systems Ba3W M □O9?x/2x?2 with MV = Nb, Ta In the system Ba3WNb□O9?x/2x/2 stacking polytypes of rhombohedral 9 L type (sequence (hhc)3; space group R3 m) can be prepared with ~1/3 ? × ? 2. For x = 2(Ba3Nb2□O8□) two modifications are formed. In the corresponding Ta system the phase with is reduced to a smaller region with x ? 1/3.  相似文献   

14.
On Hexagonal Perovskites with Cationic Vacancies. XXVII. Systems Ba4?xSrxBIIRe2□O12, Ba4B CaxRe2□O12, and Ba4?xLaxBIIRe2?xWx□O12 with BII = Co, Ni In the systems Ba4?xSrxBIIRe2□O12, Ba4BCaxRe2□O12 and Ba4?xLaxBIIRe2?xWx□O12 (BII = Co, Ni) hexagonal perovskites with a rhombohedral 12 L structure (general composition A4BM2□O12; sequence (hhcc)3; space group R&3macr;m) are observed. With the exception of Ba4NiRe2□O12 the octahedral net consists of BO6 single octahedra and M2□O12 face connected blocks (type 1). In type 2 (Ba4NiRe2□O12) the M ions are located in the single octahedra and in the center of the groups of three face connected octahedra. The two outer positions of the latter are occupied by B ions and vacancies in the ratio 1:1. The difference between type 1 and 2 are discussed by means of the vibrational and diffuse reflectance spectra.  相似文献   

15.
On Hexagonal Perovskites with Cationic Vacancies. VII. Vibrational Spectroscopie investigations on the Rhombohedral 12 L-Stacking Polytypes Ba4BII(Re2□O12) and Ba4B □1/3 (Re2 □ O12) For the rhombohedral 12 L stacking polytypes Ba4BII(Re2□O12) and Ba4B□1/3(Re2□O 12), space group R3 m, sequence (3)(1), the lattice consists of groups of three face sharing octahedra with the composition Re2□O12. They are isolated from each other by the Ba and B ions.The vibrational spectra are interpreted according to the factor group analysis. For the Re2□O12 unit (symmetry D3d) the results of a complete vibrational analysis and the calculation of the force constants are reported.  相似文献   

16.
On Hexagonal Perovskites with Cationic Vacancies. XXVI. Ba12Ba2 2/3M 1/32O333 (MV = Nb, Ta) – the First Stacking Polytypes of a Rhombohedral 36 L-Type In the systems BaO? MO5(MV = Nb, Ta) for a Ba:MV ratio of 2:1 polymorphism is observed. Here the low temperature modifications are described. They crystallize in a rhombohedral 36 L structure with three formula units Ba12Ba2 2/3M 1/32O333 for the trigonal setting (MV = Nb: a = 5.922 Å; c = 93.25 Å; Ta: a = 5,922 Å; s = 93.4 Å).  相似文献   

17.
On Hexagonal Perovskites with Cationic Vacancies. XVII. Structure Determination on Ba9Nb6W□2O27 – the First Stacking Polytype of a Rhombohedral 27 L-Type The hexagonal stacking polytype of rhombohedral 27 L -type, Ba9Nb6W□2O27, crystallizes in the space group R3 m with the sequence (4)1(3)1 ? (hhccchhcc)3 and three formula units for the trigonal setting. The refined, intensity related, R'-value is 9.7percnt;. The octahedral net consists of blocks of three face connected octahedra which are linked to each other alternately through one or two octahedra connected exclusively by common vertices. The cationic vacancies are located in the centers of the groups of three octahedra. With this distribution direct contact between occupied face-sharing octahedra is avoided. The niobium and tungsten atoms are distributed statistically between the remaining octahedral holes. In the blocks of three octahedra they are displaced by ≈ 0.29 Å from their ideal positions in the direction of the central void. The Ba atoms neighbouring a vacancy (all in hexagonal packed BaO3 sheets) are dislocated in the direction of the void, while the cubic packed BaO3 sheets maintain nearly regular form.  相似文献   

18.
On Ordered Perovskites with Cationic Vacancies. II. The Incorporation of NbV in Ba2Gd0,670,33UO6 In Ba2Gd0.670.33UO6 a complete substitution of UVI by NbV is possible by filling the cationic vacancies (x-phase: Ba2Gd0.67+0.33xU1?xNbxO6). For the y-Phase (Ba2Gd0.67U1?yNbyO6?0.5y) solid solutions are formed only for y ? 0.5. The properties of both phases are studied by x-ray and spectroscopic methods. In Ba2GdNbO6 – in contrary to the complete ordered Ba2GdTaO6 – the order of gadolinium and niobium id partial.  相似文献   

19.
On Hexagonal Perovskites with Cationic Vacancies. XIV. The Rhombohedral 12 L-Stacking Polytypes Ba2La2BII(W □O12) Rhombohedral 12 L-stacking polytypes with cationic vacancies of type Ba2La2BII-(W□O12) are reported for BII = Mg, Zn (white), Ni(light brown) and Co(brown). They crystallize in the space group R3 m, sequences (3 )(1) ? (hhcc)3. For BII = Cu, as a consequence of the Jahn Teller effect, a triclinic distorted lattice is observed.  相似文献   

20.
On ordered perovskites with cationic vacancies. VIII. Structure investigations on Ba2Ba7/81/8UO57/81/8 The reddish brown Ba2Ba7/81/8UO57/81/8 belongs to the group of oxygen perovskites with an ordered distribution of cationic vacancies. It crystallized tetragonally (a = 12.624 Å; c = 17.534 Å) with 16 formula units in the unit cell: Ba32Ba142U16O942. For the space group I4/mmm intensity calculations on powder data gave a refined, intensity related R′ value of 13.4%. The octahedrally coordinated barium an uranium atoms are 1:1 ordered; both cationic vacancies are located in the barium sublattice and form a body centered arrangement. For the 94 oxygen atoms and the two oxygen vacancies a statistical distribution was chosen. In the lattice all cations neighbouring the cationic vacancies are dislocated: The corresponding barium atoms in the close packed sheets move by ~0.55 Å in direction of the holes, on the contary the uranium atoms concerned are shifted away by ~0.17 Å and ~0.26 Å respectively.  相似文献   

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