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1.
On the Existence of Polynary Oxides of the Alkali Metals with Monovalent Cobalt and Nickel For the first time we obtained RbNa2NiO2, KNa2NiO2, Na3CoO2 and K3CoO2 [RbNa2NiO2: Na2NiO2 + Rb2O, Rb:Ni = 1.8:1, 600°C, 28 d, Ni-tube; KNa2NiO2: Na2NiO2 + K2O, K:Ni = 1.8:1, 600°C, 20 d, Ni-tube; Na3CoO2: Na2O + CoO: Na:Co = 8.8:1, 500°C, 20 d, Co-tube; K3CoO2: K2O + CoO: K:Co = 4.4:1, 550°C, 20 d, Co-tube]. According to X-ray structure analysis of single crystals monovalent Co and Ni is present [always four-circle-diffractometer data, MoKα -radiation; RbNa2NiO2: AED 2, all 163 Io(hkl), R = 3.4%, Rw = 1.9%, I4/mmm, a = 461.7(1), c = 973.6(3) pm, Z = 2; KNa2NiO2: AED 2, all 341 Io(hkl), R = 5.6%, Rw = 3.5%, Cmma, a = 1 048.5(3), b = 626.8(1), c = 621.9(1) pm, Z = 4; Na3CoO2: PW 1 100, 517 of 568 Io(hkl), R = 2.9%, Rw = 1.8%, P42/mnm, a = 940.0, c = 464.5 pm, Z = 4; K3CoO2: PW 1 100, all 940 Io(hkl), R = 5.0%, Rw = 3.9%, Pnma, a = 1 190.0, b = 730.4, c = 604.1 pm, Z = 4]. All samples are red, the single crystals transparent. Two O2? coordinate Ni1+ and Co1+, respectively, like a dumb-bell. Mean Fictive Ionic Radii, MEFIR, and Effective Coordination Numbers, ECoN, and Madelung part of lattice energy, MAPLE, are given.  相似文献   

2.
The First Oxocobaltate(II) with Dinuclear Anion: Rb2Na4[Co2O5] and K2Na4[Co2O5] By heating of well ground mixtures of the binary oxides [A2O, Na2O, ?CoO”?, A:Na:Co = 1.00:2.00:1, (A = K, Rb); Ag-tube, 600°C, 14 d] we obtained Rb2Na4[Co2O5] and K2Na4[Co2O5] rough, transparent, red single crystals. We find a new type of structure with the anion [O2CoOCoO2]6?. Space group P42/mnm; a = 634.4 pm, c = 1030.3 pm, Z = 2 (A = K) a = 647.6 pm, c = 1021.1 pm, Z = 2 (A = Rb); four-circle diffractometer data; MoKα -radiation; 360 from 364 I0(hkl), R = 4.34%, Rw = 3.54% (A = K); 361 from 366 I0(hkl), R = 6.54%, Rw = 2.70% (A = Rb). The anion is planar, the CN of Co is 3. The Madelung Part of Lattice Energy, MAPLE, and Effective Coordination Numbers, ECoN, are calculated and discussed.  相似文献   

3.
Preparation of Crystal Structure of K6[Al2O6] and Rb6[Al2O6] Colourless single crystals of K6[Al2O6] have been prepared from intimate mixtures of KAlO2 and K2O (550°C, 90 d). The structure determination from four-circle diffractometer data (MoKα , 742 Io(hkl), R = 2.2%, Rw = 2.1%) confirms the space group C2/m with Z = 2; a = 698.25 pm, b = 1 103.54 pm, c = 646.49 pm, β = 102.49°. Colourless single crystals of hitherto unknown Rb6[Al2O6] have been prepared from intimate mixtures of RbAlO2 and Rb2O (520°C, 120 d). The structure determination from four-circle diffractometer data (MoKα , 1 240 Io(hkl)) results in the residual values R = 7.2%, Rw = 4.9%; space group C2/m; a = 725.92 pm, b = 1 143.33 pm, c = 678.06 pm, β = 104.05°; Z = 2. K6[Al2O6] and Rb6[Al2O6] are isostructural with K6[Fe2O6]. A characteristic structure unit is the anion [Al2O6]6? consisting of two edge-sharing [AlO4] tetrahedra. Effective Coordination Numbers (ECoN), Mean Fictive Ionic Radii (MEFIR), the Madelung Part of Lattice Energy (MAPLE) and the Charge Distribution (CHARDI) are calculated and discussed.  相似文献   

4.
The First Oxocobaltate of the Type A2CoIIO2: K2CoO2 = K4[OCoO2CoO] By “reaction with the cylinder surface” of intimate mixtures of K2O and CdO (molar ratio 1:1) in closed Co-Cylinders at 450°C during 73 d dark-red single-crystals of K2CoO2 were obtained. Structure solution and refinement (four-circle diffractometer-data, MoKα , 1 567 independent Io(hkl), none was omitted, R = 3.25%, Rw = 2.67%) result in a monoclinic unit cell containing anions [Co2O4]4? of two connected triangles similar to those of Rb10[CoIO2]2[CoO4]. MAPLE-values and Charge-distributions are given and discussed.  相似文献   

5.
What does Solid State Mean?. New Molecular Aspects on the Example of Rb2[TiO3] [1], [2] Rb2TiO3 [3], parent type of the oxides K2CoO3, Rb2CoO3 and Cs2CoO3 [4], colourless crystals, needles, was newly obtained by heating a well grounded mixture of the binary oxides RbO0.98, RbO0.52, Ti2O3 (molar ratio = 2.4:6.2:1.0) 41 d at 780°C in Ni-Tubes. The first structure determination by using four-circle diffractometer data (Siemens AED2, 5366 Io(hkl), MoKα ) leads to the residual-values R = 7.9% and Rw = 3.7%. Lattice constants (orthorhombic, Cmca, Z = 8, Guinier-Simon-data, CuKα1): a = 596.5(1) pm, b = 1185.2(1) pm, c = 1326.6(1) pm (additional data see text). The structure determination 1974 by filmdata is confirmed. The Madelung Part of Lattice Energy (MAPLE), Effective Coordination Numbers (ECoN), Mean Fictive Ionic Radii (MEFIR) and the Charge Distribution in Solids (CHARDI) are calculated and discussed.  相似文献   

6.
New Oxides with the “Butterfly-Motive”: Rb6[Fe2O5] and K6[Fe2O5] Rb6[Fe2O5] and K6[Fe2O5] were obtained for the first time by annealing intimate mixtures of “Rb6CdO4” with CdO (molar ratio 1 : 1.1) and KO0.48 with CdO (molar ratio 5.9 : 1) respectively in closed Fe-cylinders. Determination and refinement of the crystalstructure confirms the space group C2/m (four-circle-diffractometer data). Rb6[Fe2O5]: Ag Kα , 720 out of 1220 Io(hkl), R = 9.68%, Rw = 6.09%; a = 718.9pm, b = 1183.1 pm, c = 695.4pm, β = 95.05°, Z = 2; K6[Fe2O5]: MoKα , 1214 Out of 12141o(hkl), R = 3.20070, Rw = 2.48%, a = 691.21 pm, b = 1142.78pm, c = 665.50pm, β = 93.82°, Z = 2. The binuclear unit [O2FeOFeO2]6? already known to be planar with oxoferrates(II) now was observed to be angular here and closely related to Na6[Be2O5].  相似文献   

7.
On K2Na4[O2BeOBeO2] For the first time colourless single crystals of K2Na4[Be2O5] which are isotypic with K2Na4[Co2O5] [2] and Rb2Na4[Co2O5] have been prepared by heating e.g. a well ground mixture of K2O, Na2O and BeO (K:Na:Be = 2.2:4.4:2; 750°C; 21 d; Ni-tube). The crystal structure was solved by four-circle diffractometer data [Siemens AED 2; 389 Io(hkl); space group P42/mnm; Z = 2; a = 595.17(4) pm, c = 1 002.66(9) pm; R = 4.1%; Rw = 2.3%]. Mean Fictive Ionic Radii, MEFIR, Effective Coordination Numbers, ECoN, the Madelung Part of Lattice Energy, MAPLE, and the charge distribution are calculated.  相似文献   

8.
The First Oligooxoindate(III): K14[In4O13] For the first time K14[In4O13] was obtained by heating intimate mixtures of K2O, CdO and elementar In (molar ratio 3.1:1.0:1.0) in closed Ag-cylinders (30 days, 450°C) in form of yellow-brown single crystals. The structure determination by four circle diffractometer data MoKα, 3 689 out of 3 689 Io(hkl), R = 4.22, Rw = 2.45) confirms the space group P21/c with lattice constants a = 687.7 pm; b = 3 118.5 pm; c = 686.4 pm; β = 119.3°; Z = 2. The characteristic feature of the structure is [In4O13]14? groups, oligomers consisting of four corner-sharing InO4 tetrahedra. These groups are connected by crystallographically distinct potassium atoms. The structure is isotypic with Na14[Al4O13] [2] and K14[Fe3O13] [3]. ECoN and MAPLE calculationes are discussed.  相似文献   

9.
A New Cobaltate with Isolated Anion Structure: Li6[CoO4] For the first time transparent, blue single crystals of Li6[CoO4] have been prepared (Li2O/Na2O/?CoO”? (Li:Na:Co = 1.3:1.3:1), Co-tube, 580°C, 22 d). Corresponding to Li6□CoO; it is an ordered variant of the Li2O-type of structure: P42/nmc; a = 653.6(1) pm, c = 465.4(1) pm; Z = 2; dx = 2.75 g cm?3, dpyk = 2.71 g cm?3 (4-circle-diffractometer-data (PW 1100), AgKα; 230 from 936 I0(hkl); R = 9.58%, RW = 5.25%). Parameters see text. The Madelung Part of Lattice Energy, MAPLE, and Effective Coordination Numbers, ECoN, these via Mean Fictive Ionic Radii, MEFIR, are calculated and discussed. The magnetic properties are measured in the temperature range of 14–297 K.  相似文献   

10.
On ?Lithovanadates”?: Rb2[LiVO4] and Cs2[LiVO4] By heating of well ground mixtures of the binary oxides [A2O, Li2O, V2O5, A : Li: V = 2.2 : 1.1 : 1.0 (A = Rb, Cs); Ni-tube, 750° 25 d] we obtained Rb2[LiVO4] and Cs2[LiVO4] colourless, orthorhombic single crystals. We found a new type of ?Lithovanadate”?-structure: space group Cmc21; a = 587.9(1), b = 1170.1(1), c = 793.3(1) pm, Z = 4 (A = Rb) bzw. a = 610.5(1), b = 1222.6(3), c = 815.5(2) pm, Z = 4 (A = Cs). The structure was determined by four-circle diffractometer data [MoKα -radiation; 997 from 1157 I0(hkl), R = 7.75%, Rw = 5.54% (A = Rb); 686 from 686 I0(hkl), R = 6.97%, Rw = 4.20% (A = Cs)] parameters see text. The Madelung part of Lattice Energy, MAPLE, and Effective Coordination Numbers, ECoN, these via Mean Fictive Ionic Radii, MEFIR, have been calculated.  相似文献   

11.
The First Oxoferrate(I): On the Constitution of K3[FeO2] and K3[NiO2] Garnet-red single crystals of K3[FeO2] were obtained for the first time by heating intimate mixtures of K6[CdO4] and CdO (molar ratio 1:1.16) in closed Fe-cylinders at 450°C during 40 d. The same way of preparation via “reaction with the cylinder surface” was applied to prepare similarly coloured single crystals of K3[NiO2] (K6CdO4 in closed Ni-cylinders at 500°C during 49 d). The structure determination by four circle diffractometer data (MoKα , K3[FeO2]: 731 out of 731 Io(hkl), R = 5.76%, Rw = 5.33%, K3[NiO2]: 755 out of 755 Io(hkl), R = 8.70%, Rw = 4.25%) confirms the space groups P 41212 and P 43212, respectively. K3[FeO2]: a = 604.2(2) pm, c = 1 402.7(3) pm, Z = 4 K3[NiO2]: a = 603.6(1) pm, c = 1 405.2(2) pm, Z = 4. (powder data, standard deviations in parentheses) Essential feature of the structure are the dumb-bell-like anions [O? M? O]3? (M = Fe, Ni). Their arrangement corresponds to a stuffed derivative of the KrF2-type. Magnetic properties of K3[FeO2] were determined and cover the monovalence of Fe. MAPLE-calculations reveal the strong coincidence of monovalent VIIIb-cations.  相似文献   

12.
Inhaltsübersicht. Erstmals wurden klar durchscheinende, orange-farbene Einkristalle von Cs2Li14[Tb3O14] aus Cs2TbO3 und Li2O (Tb: Li = 1:5) dargestellt [550°C, 21 d, verschlossenes AuRohr]. Es liegt der K2Li14[Pb3O14]-Typ vor [Vierkreisdiffraktometerdaten, PW 1100, MoKä-Strahlung, 660 Io(hkl), R = 4,8%, Rw = 3,4%, Immm, a = 1293,5(8), b = 792,6(3), c = 740,4(3) pm, Z = 2, d = 4,65]. Ebenfalls neu wurde K2Li14[Zr3O14] in Form farbloser Einkristalle durch Tempern inniger Gemenge von K2O, Li2O und ZrO2 (K: Li: Zr = 1:4:1,5) dargestellt [900°C, 14 d, geschlossene Ni-Bombe] und röntgenographisch untersucht. Die Strukturverfeinerung [612 Io(hkl), Vierkreisdiffraktometerdaten, PW 1100, MoKα-Strahlung, R = 5,9%, Rw = 5,3%, Immm, a = 1244,6, b = 776,4, c = 724,3 pm, Z = 2] bestätigt die Isotypie mit K2Li14[Pb3O14]. Der Madelunganteil der Gitterenergie, MAPLE, Effektive Koordinationszahlen, ECoN, diese über Mittlere Effektive Ionenradien, MEFIR, wurden berechnet. Für die nun bekannten Vertreter dieses Typs wurde ein Isotypievergleich vorgenommen. New Compounds of the K2Li14[Pb3O14] Type: Cs2Li14[Tb8O14] and K2Li14[Zr3O14] For the first time Cs2Li14[Tb3O14] has been prepared as orange single crystals from Cs2TbO3 and Li2O (Tb: Li = 1:5) [550°C, 21 d, sealed Au-Tube]. Structure Refinement [four-circle diffractometer data, PW 1100, MoKα radiation, 660 Io(hkl), R = 4.8%, Rw = 3.4%, Immm, a = 1293.5(8), b = 792.6(3), c = 740.4(3) pm, Z = 2, d = 4.65] confirms isotypy with K2Li14[Pb3O14]. K2Li14[Zr3O14] has also been prepared as colorless single crystals from K2O, Li2O, and ZrO2 (K: Li: Zr = 1:4:1.5), [900°C, 14 d, closed Ni-cylinder] and investigated by x-ray [612 Io(hkl), four-circle diffractometer data, PW 1100, MoKα radiation, R = 5.9%, Rw = 5.3%, Immm, a = 1244.6, b = 776.4, c = 724.3 pm, Z = 2]. The Madelung Part of Lattice Energy, MAPLE, and Effective Coordination Numbers, ECoN, the latter derived from Mean Effective Fictive Ionic Radii, MEFIR, are calculated. A detailed comparison of the structures is carried out.  相似文献   

13.
A New ?Orthoindate”? of an Alkali Metal: K5[InO4] Hitherto unknown K5[InO4] was prepared by heating intimate mixtures of K2O, In2O3 and elementar In (molar ratio 10.0 : 1.0 : 4.0) in closed Ni-cylinders (30 days, 500°C) in form of pale red, nearly colourless, transparent, single crystals. Same crystals were obtained by heating mixtures of K2O, CdO and elementar In (molar ratio 3.1 : 1.0 : 1.0) in closed Ag-cylinders (30 days, 450°C), too. In this case we also found yellow-brown crystals of K14[In4O13] [1]. Structure determination by four circle diffractometer data (MoKα, 15279 out 17454 Io(hkl), R = 5.60%, Rw = 5.25%). Space group P1 with a = 1827.9 pm; b = 1694.4 pm; c = 1329.4 pm; α = 113.3°; β = 111.4°; γ = 105.2°; Z = 16. Characteristic feature of the structure are isolated [InO4]5?-tetraeder. The Madelung Part of Lattice Energy, MAPLE, the Mean Fictive Ionic Radii, MEFIR, Effective Coordination Numbers, ECoN, and Charge Distribution, VADI, are calculated.  相似文献   

14.
About Cs2Li2[GeO4] By heating of a well-ground mixture of the binary oxides CsO0.55, Li2O and GeO2 (Cs:Li:Ge=2,6:2,2:1; Ni-tube; 600 °C; 49d) we got single crystals of Cs2Li2[GeO4] for the first time. Cs2Li2[GeO4] is isotypic to Rb2Li2[MO4] [M = Si, Ti, Ge] [2] and Cs2Li2[MO4] (M = Si, Ti) [3]: according to this Cs2Li2[GeO4] crystallizes triclinic, in the spacegroup P1 with a = 968.7(4) pm, b = 586.0(2) pm, c = 571.4(2) pm, α = 92.71(4)°, β = 110.95(3)° and γ = 94.34(4)° (Guinier-Simon data), Z = 2. The structure was determined by four-circle diffractometer data (Ag? Kα ; 2381 Io(hkl); R = 8,4%; Rw = 5.0%), parameters see text. Further the Madelung Part of Lattice Energy (MAPLE), Effective Coordination Numbers (ECoN) and the Mean Fictive Ionic Radii (MEFIR), have been calculated.  相似文献   

15.
Cs4[IrO4], a New Iridate with Planar Anion [IrO4]4? For the first time we obtained black single crystals of Cs4[IrO4] by heating intimate mixtures of CsO0.52 and IrO2 (molar ratio Cs : Ir = 4.30 : 1.00; “Ag-bomb”, 740°C/86 d). Cs4[IrO4] crystallizes monocline, C 2/m, with a = 1031.66(8) pm, b = 671.61(4) pm, c = 660.44(6) pm, b? = 108.118(7)° and Z = 2 in the K4[IrO4]-type. The structure has been determined by four-circle-diffractometer data (PW 1100 from Phillips, Ag? Kα , graphite) with 841 I0(hkl) with I ≥ 3s?(F) (from 947 I0(hkl) out of 3529 measured reflexes). The Madelung Part of Lattice Energy, MAPLE, Effective Coordination Numbers, ECoN, these via Mean Fictive Ionic Radii, MEFIR, are calculated and discussed.  相似文献   

16.
New Metal Oxides with Doubles of Tetrahedra as Building Units: Rb6[Tl2O6] and Cs6[In2O6] We prepared the hitherto unknown Rb6[Tl2O6] and Cs6[In2O6] by heating mixtures of Tl2O3 and RbO0.60 (Rb:Tl = 3.5:1) as well as In2O3 and CsO0.53 (Cs:In = 3.5:1) as single crystals [closed Ag-cylinder, 650°C, 14 d]. The single crystals of Rb6[Tl2O6] are yellow, those of Cs6[In2O6] pale yellow, all transparent and rude. The new type of structure was elucidated by 4-circle-diffractometer (PW 1100) data. Rb6[Tl2O6]: P21/a; a = 1145,7(3), b = 713,3(1), c = 783,9(2) pm, β = 93,73° (2), Z = 2; Ag–Kα, 2100 out of 2531 I0(hkl), R = 9,6% and Rw = 8,9%. Cs6[In2O6]: P21/a; a = 1178,5(4), b = 730,7(2), c = 816,3(2) pm, β = 95,38° (3), Z = 2; Mo–Kα, 1584 out of 2032 I0(hkl), R = 9,25%, and Rw = 8,44%. The Madelung Part of Lattice Energy, MAPLE, is calculated and discussed.  相似文献   

17.
The Crystal Structure of KGaO2 and NaGaO2(II) By annealing intimate mixtures of K2O, Na2O and β-Ga2O3 (K : Na : Ga = 2.2 : 1.1 : 1) we obtained single crystals of K2Na4[(GaO3)2] and KGaO2 (Ag-cylinder; 600°C, 26 d). Structure refinement for KGaO2 (four-circle diffractometer data, Mo-Kα , 1 390 or 1 390 Io(hkl); R = 5.55%, Rw = 3.05%) confirms the space group Pbca; a = 552.1 pm, b = 1 107.5 pm, c = 1 580.7 pm, Z = 16. According to K[GaO4/2] we have a stuffed cristobalite-related structure. Single crystals of NaGaO2(II) were grown by annealing intimate mixtures of Na2O2 and GaAs (Na2O2 : GaAs 4.1 : 1) in Ag-cylinders that were not completely closed (570°C, 6 weeks). Structure refinement for NaGaO2(II) (four-circle diffractometer data, Mo-Kα , 588 of 616 Io(hkl); R = 4.54%, Rw = 4.06%) confirms the spacegroup Pna21; a = 549.8(1) pm, b = 720.6(1) pm, c = 529.8(1) pm, Z = 4. In NaGaO2(II) we have a wurtzite-related structure.  相似文献   

18.
The First Tetraferrate(III): K14[Fe4O13] For the first time K14[Fe4O13] was obtained by annealing intimate mixtures of K2O and LiFeO2 (molar ratio 2.2:1) in closed Ni-cylinders (6 months, 610°C) in the form of yellow-brown single crystals. The structure determination (four circle diffractometer, MoKα, 3377 of 3377 Io(hkl); R = 4,52%, Rw = 2,53%) confirms the space group P21/c; a = 677.9, b = 2956.2, c = 672,1 pm, β = 120.31°, Z = 2. Essential part of the structure are tetranuclear [Fe4O13]14?-groups, oligomers consisting of four corner-sharing FeO4-tetrahedra. Within the structure these groups are connected by two crystallographically distinct K-particles thus forming bands which are arranged according to a ?closest packing of bands”? interconnected by the rest of the K-particles. The structure is described via Schlegel-diagrams. It is isotypic with Na14[Al4O13].  相似文献   

19.
On K4PbO4 and Rb4PbO4 For the first time single crystals of K4[PbO4] have been prepared by heating K4PbO3 in O2. The structure has been refined [K4[PbO4]: 3029 I0(hkl), four circle diffractometer PW 1100, ω-scan, MoKα, R = 6.73%, Rw = 6.64%, P1 ; a = 658.62(15), b = 658.41(12), c = 986.64(21) pm, α = 79.74(2)°, β = 108.45(2)°, γ = 112.49(2)°, dx = 3.79 g · cm?3, dpyk = 3.78 g · cm?3, Z = 2; Rb4[PbO4]: a = 686.94(18), b = 684.43(18), c = 1020.73(21) pm, α = 79.28(2)°, β = 108.40(2)°, γ = 113.02(2)°, dx = 4.87 g · cm?3, dpyk = 4.85 g · cm?3, Z = 2, (from Rb2PbO3 and Rb2O)]. Both compounds are isotypic with K4SnO4. The Effective Coordination Numbers, ECoN, these via Mean Fictive Ionic Radii, MEFIR, are calculated.  相似文献   

20.
A New Oxogermanate: Li8GeO6 ? Li8O[GeO4] Transparent colourless single crystals of Li8GeO6(P63cm, a = 550.09(8), c = 1072.2(3) pm, Z = 2; 4-circle-diffractometer Siemens AED 2, MoKα; 326 Io(hkl), R = 2.4%, Rw = 2.0%), have been prepared. As by-product we always got colourless isometric single crystals of Li4GeO4. For the first time we could grow single crystals of Li8SiO6 of suitable size and quality. Our structure refinement confirms the assumed structure model [2]: Li8GeO6 and Li8SiO6 are isotypic with Li8CoO6[3] (Li8SiO6: a = 542.43(8), c = 1062.6(2) pm, Z = 2; 4-circle-diffractometer Siemens AED 2, MoKα; 306 Io(hkl), R = 3.6%, Rw= 3.0%). The known crystal structure of Li4GeO4 [4] is confirmed and refined (Cmcm, a = 776.6(2), b = 735.7(3), c = 604.9(2) pm, Z = 4; 4-circle-diffractometer Siemens AED 2, MoKα, 298 Io(hkl), R = 1.9%, Rw = 1.4%). The Madelung Part of Lattice Energy, MAPLE, and Effective coordination-Numbers, ECoN, these via Mean Fictive Ionic Radii, MEFIR, are calculated.  相似文献   

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