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Li2SnO3 crystallises monoclinic, C, with a = 5.295, b = 9.184, c = 10.032 Å and β = 100.13°; Z = 8. The positions of Sn were obtained from PATTERSON maps and the positions of O and Li by FOURIER difference method. Parameters were refined by least squares-method [1462 reflexes (h 01)–(h 71); R = 10.5%]. The average distances of Li? O are 2.07 Å, and 2.20 Å for Sn? O. The Li2SnO3 structure can be derived from the NaCl type: in a cubic closest packing of oxygen 2/3 of the octahedral holes are occupied by lithium and 1/3 by tin. 相似文献
4.
Magnetochemistry of Divalent Silver. New Fluoroargentates(II): Cs2AgF4, Rb2AgF4, and K2AgF4 Hitherto unknown blue compounds Rb2AgF4 and Cs2AgF4 are prepared. Guinier patterns show, that Cs2AgF4 cristallise in the K2NiF4 structure (a = 4.581, c = 14.192 Å). The structure of the Rb-compound is still unknown. The magnetic behaviour of K2AgF4, Rb2AgF4, and Cs2AgF4 is discussed. 相似文献
5.
New Nesozincates: K4[ZnO3], Rb7Na[ZnO3]2 For the first time A) K4[ZnO3] and B) Rb7Na[ZnO3]2 have been prepared (from the binary oxides). They represent the first oxozincates of the alkali metals in which the coordination number of Zn2+ is exclusively 3 (carbonate-like groups [ZnO3]). Both oxides crystallize triclinic, space group P1 with A): a = 1103.3(3), b = 881.3(3), c = 698.2(2) pm, α = 109.65(2)°, β = 89.56(2)°, γ = 102.41(3)° and Z = 4, and B): a = 1128.3(3), b = 974.5(3), c = 711,8(2) pm, α = 114.12(2)β, = = 88.46(3)°,γ = 106.48(2)° and Z = 4. Their crystal structures have been determined from single crystal data (four circle diffractometer) and refined to R = 10.1%, Rw = 7.8% (2905 unique I0(hkl)) and R = 19.5%, Rw = 17.3% (2269 unique I0(hkl)), respectively. The Madelung Part of Lattice Energy (MAPLE), Effective Coordination Numbers (ECoN) and Mean Fictive Ionic Radii (MEFIR) have been calculated. 相似文献
6.
About Perrhenates. 1. On LiReO4 For the very first time anhydrous LiReO4 was prepared in transparent, colourless single crystals from Li2O2 and Re2O7 (closed Au-pipe; 350°C; 14 d). The crystal structure, P1 , with a = 9.652(1), b = 8.455(1), c = 6.928(1) Å, α = 101,53° (1), β = 106.55° (1), γ = 97.22° (1), Z = 6, dx = 4.92 g/cm3, dpyk = 4,81 g/cm3 was solved (four-circle-diffractometer data PW 1100, 2151 I0 (hkl), AgKα; R = 0.073, Rw = 0.076). There are three kinds of functionally different Li+. The Madelung Part of the Lattice Energy, MAPLE, was calculated. 相似文献
7.
Thermal Behaviour of Li3MnO4. II. α- and β-Li2MnO3 By thermal decomposition of Li3MnO4 we obtained two new forms of Li2MnO3: α-Li2MnO3 crystallizes due to Guinier-Simon photographs cubic face-centered with a = 4.092 Å, β-Li2MnO3 hexagonal with a = 4,93, c = 14.24 Å, c/a = 2.89. α-Li2MnO3 is paramagnetic with μ = 3,82 B.M. Below the Neel temperature (≈? 50 K) β-Li2MnO3 is antiferromagnetic. Effective Coordination Numbers, ECoN, are calculated and discussed. 相似文献
8.
New Investigations about Oxo Uranates: On α-Li6UO6. With a Remark about β-Li6UO6 The crystal structure of transparent, bright yellow single crystals of α-Li6UO6 has been determined. [a = 838.07(5), c = 738.34(7) pm; dpyk = 4.02, dx = 4.17 g · cm?3; space group R3 ; Z = 3; R = 3.17%, Rw = 3.06%; 408 symmetry independent I0(hkl); AgKα fourcircle diffractometer Philips PW 1100]. The structure is dominated by a threedimensional framwork of “hollow spaces”, built up by 12 O2? (and 12 Li+). The Madelung Part of Lattice Energy, MAPLE, is calculated and discussed. 相似文献
9.
[reaction: see text]. The alpha-deprotonation of alkynyl carbamates 3 with the chiral base (-)-sparteine (4)/n-butyllithium, transmetalation with ClTi(O(i)()Pr)3, and subsequent substitution with an aldehyde results in the formation of enantioenriched 4-hydroxyallenyl carbamates 11. Stereoselection is determined by dynamic resolution of the lithium/(-)-sparteine complexes by selective crystallization. 相似文献
10.
Note on Li2PdO2 For the first time we prepared ruby-red single crystals of Li2PdO2 by reaction with the wall 3 Na2O + Li2O2 + ?Tb4O7”?(+ Pd) = 3 Na2TbO3 + Li2PdO2 + ?TbO2”?, Pd-tube, 1100°C, 7 d. Single crystal data confirm the Li2CuO2-type of structure [a = 375.34(5), b = 298.18(4), c = 931.58(10) pm; spacegroup Immm; dx = 4.85 g · cm?3; 144 I0(hkl); R = 3.54%, Rw = 3.19%; MoKα ; four-circle diffractometer Philips PW 1100] and reveal clearly different parameters compared with those deduced by powder data. The Madelung Part of Lattice Energy, MAPLE, corresponds now to the sum of the MAPLE values of the binary oxides. 相似文献