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1.
More Silicates with ?Stuffed Pyrgoms”?: CsKNaLi9{Li[SiO4]}4, CsKNa2Li8{Li[SiO4]}4, RbNa3Li8{Li[SiO4]}4 [1] and RbNaLi4{Li[SiO4]}2 [2] Single crystals of the new silicates CsKNaLi9{Li[SiO4]}4, CsKNa2Li8{Li[SiO4]}4, RbNa3Li8{Li[SiO4]}4 and RbNaLi4{Li[SiO4]}2 as well as powder (Rb-containing compounds only) were obtained for the first time. The samples were prepared by heating well ground mixtures of the binary oxides in Ni and Ag tubes, respectively. The structure determination was carried out by four-circle diffractometer data (MoKα radiation; Siemens AED 2): CsKNaLi9{Li[SiO4]}4: tetragonally prismatic crystals, light yellow; 726 I0(hkl), R = 4.4%, Rw = 2.8%; a = 1 102.0(6), c = 637.9(5) pm; Z = 2; space group I4/m; 2 CsO0.55 + Li4TlO4 + glas (560°C, 15 d). CsKNa2Li8{Li[SiO4]}4: tetragonally prismatic crystals, light yellow; 727 I0(hkl), R = 4.4%, Rw = 2.6%; a = 1 103.5(7), c = 637.7(4) pm; Z = 2; space group I4/m; 1.1 CsO0.61 + 1.1 KO0.55 + 1.4 NaO0.52 + 6.5 Li2O + 4 SiO2 (600°C, 60 d). RbNa3Li8{Li[SiO4]}4: tetragonally prismatic crystals, colourless; 600 I0(hkl), R = 2.3%, Rw = 2.0%; a = 1 092.08(6), c = 632.76(4) pm; Z = 2; space group I4/m; 4 RbO0.57 + 3 NaO0.52 + 6.5 Li2O + 4 SiO2 (650°C, 63 d). RbNaLi4{Li[SiO4]}2: monoclinic, ball-shaped, colourless; 1 224 I0(hkl), R = 3.1%, Rw = 3.1%; a = 1 573.10(13), b = 630.48(5), c = 781.25(8) pm, b = 90.566(8)°; Z = 4; space group C2/m; 1.1 RbO0.52 + 1.2 NaO0.45 + 5 Li2O + 4 SiO2 (700°C, 40 d).  相似文献   

2.
The First Oxogermanate with “Stuffed Pyrgoms”: CsNa3Li8{Li[GeO4]}4 By heating the binary oxides CsO0.52, NaO0.45, LiO0.5 and GeO2 in the mol. ratio 1.24:1.4:6.7:3.9 (Ni tubes; 600°C/89 resp. 65 d) we obtained for the first time CsNa3Li8{Li[GeO4]}4 in form of pale yellow prisms as well as powder: space group I4/m (I. T. No. 87) with a = 1 120.73(5); c = 651.64(5) pm; Z = 2; (four circle diffractometer data; MoKα; 5 152 Io(hkl); R = 1.7%; Rw = 1.6%), parameters see text. The structure determination confirmes its being isotypic with CsKNaLi9{Li[SiO4]}4, CsKNa2Li8{Li[SiO4]}4 and RbNa3Li8{Li[SiO4]}4. The Madelung part of lattice energy (MAPLE), effective coordination numbers (ECoN), mean fictive ionic radii (MEFIR) and the charge distribution (CHARDI) are calculated.  相似文献   

3.
The new lithium nitridotantalate(V), Li4[TaN3], was prepared by reaction of Li15[CrN4]2N with the wall of a welded Ta ampoule in the presence of metallic Li at 1470 K. Li4[TaN3] forms colourless single crystals (platelets, space group Ibca, No. 73, a = 491.85(4) pm, b = 973.59(6) pm, c = 1415.0(1) pm, Z = 8, R1 = 0.0288). The crystal structure is described as Li2O superstructure with ordered occupation of the tetrahedral sites by Li and Ta. The resulting arrangement leads to infinite chains [TaN2N2/24—] running along [100].  相似文献   

4.
The First “Litho-Manganate(V)” with Layer-Structure: Cs2{Li[MnO4]} By heating intimate mixtures of the oxides [CsO1,2, Li2MnO3; Cs: Mn = 2,3 : 1; Ag-Zylinder, 580°C, 62 d] blue-green single crystals of Cs2{Li[VO4]} were obtained for the first time. The new “Litho-Manganate(V)” crystallices orthorhombic (SG: Cmc21) with a = 596.08(7), b = 1202.6(1), c = 816.8(1) pm (Guinier-Simon data), Z = 4. It is isotypic with Cs2{Li[VO4]} [1]. The structure was determined by four-circle-diffractometer data [Mo? Kα , for 496Io(hkl) R = 3.1%, R, = 2.4%], parameters see text. The Madelung Part of Lattice Energie, MAPLE and Effective Coordination Numbers, ECoN, these calculated via Mean Fictive Ionic Radii, MEFIR, are calculated and disscussed.  相似文献   

5.
A “Lithosilicate” with Columnar Units: RbLi5{Li[SiO4]}2 In order to prepare RbLi3[SiO4] single crystals of RbLi5{Li[SiO4]}2 have been obtained for the first time by heating of a well ground mixture of the binary oxides RbO0.68, LiO0.5 and SiO2 [Rb:Li:Si = 1.1:3.0:1.0; 600°C; 21 d] in tightly closed Ni tubes. The new “lithosilicate” crystallizes monoclinic (space group C2/m with a = 1563.1(2) pm, b = 635.4(1) pm, c = 776.3(1) pm, β = 90.53(1)°, Guinier-Simon powder data). The crystal structure was determined by four-cycle diffractometer data [Philips PW 1100, 1237 from 1609 Io(hkl), Z = 4, R = 9.2%, Rw = 8.3%], 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   

6.
Li10Si2PbIIO10 = Li20[(SiO4)4(OPbO2PbO)] — The first ?mixed”? Silicate-Plumbate(II) Colourless crystals of Li10Si2PbO10 were obtained by heating a well-ground mixture of LiPb, Li2O2 and ?SiO2”? (deriving from Duran glas) in Ag-tubes (650°C; 60 d). The crystal structure was determined (four-circle diffractometer data, Mo? K, 1 474 Io(hkl), R = 4.2%, Rw = 2.8%, parameters see text). The silicate-plumbate crystallizes monoclinic (space group C2/m; I. T. No. 12) with a = 2985.1(4); b = 610.6(6); c = 512.8(1) pm, β = 99.70(9)° (four-circle data), Z = 4. Further the Madelung Part of Lattice Energy (MAPLE), Effective Coordination Numbers (ECoN), the Mean Fictive Ionic Radii (MEFIR) and the Charge Distribution (CHARDI) are being calculated.  相似文献   

7.
The New Orthotitanate CsNa3[TiO4] Colourless, square stonelike single crystals of CsNa3[TiO4] [1], isostructural with CsNa3[PbO4] [2], are obtained by heating a well grounded mixture of the binary oxides CsO0,56, NaO0,52 and TiO2 (Cs : Na : Ti = 1,1:3,1:1,0) in Nitubes (9d, 400°C). The structure determination by using four-circle diffactometer data (Siemens AED2, 5541 Io(hkl), MoK) leads to the residual-values R = 8.8% and Rw = 4.7%. Lattice constants (triclinic, Cmca, P1 , Z = 4, four-circle diffactometer data, MoK: a = 1161.2(6) pm, b = 854.9(3) pm, c = 651.1(3) pm, α = 100.52(2)°, β = 108.84(3)°, γ = 91.61(3)°; additional data see text). 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   

8.
A New Oxozincate: Li6[ZnO4] Colourless single crystals of Li6[ZnO4] are formed by reaction of Li2O and ZnO [(Li2O:ZnO = 3.3:1, 700°C 50 d), Space group P42/nmc, Z = 2, a = 652.76 pm, c = 465.09 pm R = 2.6%, Rw = 2.1%, 173 symmetry independend I0(hkl), MoK]. The crystal structure has been determined.  相似文献   

9.
Preparation and Crystal Structure of BaLi[BO3] For the first time colourless lamellar single crystals of BaLi[BO3] have been prepared from intimate mixtures of BaO2, Li2O and B2O3. The structure determination from four-circle diffractometer data (MoKα , 882 independent reflections, R = 2.4%, Rw = 1.9%) confirms the space group P 21/c with Z = 4; a = 646.1(3), b = 710.7(2), c = 740.3(3) pm, β = 117.99(3)°. Characteristic units of the structure are layers {Li[BO3]} parallel to (100) consisting of trigonal planar [BO3] groups and distorted [LiO5] pyramids. 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   

10.
Chains consisting of Rings: K5{Li[Ge2O7]} — the First ‘Litho-Digermanate’ By heating of a well-ground mixture of the binary oxides KO0.55, Li2O and GeO2 (K: Li: Ge = 6.1 : 2.2 : 2; Ni-tube; 600°C; 49 d) we obtained for the first time single crystals of K5{Li[Ge2O7]}. This ‘lithodigermanate’ represents a completely new type of structure: monoclinic, space group P21/c, a = 624.9(2) pm, b = 1586.6(8) pm; c = 1058.3(6) pm and β = 109.38(4)°; Guinier-Simon data, Z = 4. The structure was solved by four-circle diffractometer data [Siemens AED II, Mo? Kα ; 2872 Io(hkl); R = 4.5%, Rw = 3.3%], parameters see text. The Madelung Part of Lattice Energy, MAPLE, and Effective Coordination Numbers, ECoN, these calculated via Mean Fictive Ionic Radii, MEFIR, as well as charge distribution CHARDI, are calculated and discussed.  相似文献   

11.
New Alkalioxoarsenates (V). On Rb2Li[AsO4] and Cs2Li[AsO4] By heating of well-grounded mixtures of the binary oxides (A2O, Li2O2, and As2O3; A : Li : As = 2 : 1 : 1; Ni-tube, 550°C, 21 d; A = Rb, Cs) colourless single crystals of Rb2Li[AsO4] and Cs2Li[AsO4] were obtained for the first time. These new orthoarsenates(V) crystalize orthorhombic (space group C mc21? C, No. 36) with Z = 4. As expected they are isotypic with the according orthovanadates(V) [2] A2Li[VO4], A = Rb, Cs. The lattice constants of Rb2Li[AsO4]: a = 582.1(4) pm, b = 1171.1(7) pm, c = 792.4(5) pm and Cs2Li[AsO4]: a = 596.4(2) pm, b = 1223.4(2) pm, c = 819.7(3) pm were taken from Guinier-Simon powder data. The structure was determined by four-circle-diffractometer data [Siemens AED II, MoKα , 6290 I0 (hkl), R = 3.5%, Rw = 3.2% to Rb2Li[AsO4]; 3518 I0 (hkl), R = 2.8%, Rw = 2.6% to Cs2Li[AsO4]; parameters see text]. The Madelung Part of Lattice Energy, MAPLE, and Effective Coordination Numbers, ECoN, these calculated via Mean Fictive Ionic Radii, MEFIR, as well as charge distribution CHARDI are calculated and discussed.  相似文献   

12.
Li3InO3 crystallises trigonal, P3 c1, with a = 9.6064, c = 10.420 Å, c/a = 1.0647, Z = 12 and In1 in 2(a), In2: 4(d), In3: 6(f), and O1, O2, O3, Li1, Li2, Li3 each in 12 (g). According to Li2[4]{In□1/3}O2 Li3InO3 is a “stuffed derivative” of a layer structure of the CdJ2 type. Calculations of the Madelung Part of Lattice Energy [MAPLE] assure the localisation of Li by X-Ray work and explain why In2, O1, O2, and O3 depart from “ideal” positions.  相似文献   

13.
Tetraammine Lithium Cations Stabilizing Phenylsubstituted Zintl-Anions: The Compound [Li(NH3)4]2[Sn2Ph4] Ruby-red, brittle single crystals of [Li(NH3)4]2[Sn2Ph4] were synthesized by the reaction of diphenyltin dichloride and metallic lithium in liquid ammonia at ?35°C. The structure was determined from X-ray singlecrystal diffractometer data: Space group, P1 , Z = 1, a = 9.462(2) Å, b = 9.727(2) Å, c = 11.232(2) Å, α = 66.22(3)°, β = 85.78(3)°, γ = 61.83(3)°, R1 (F ? 4σF) = 5.13%, wR2 (F02 ? 4σF) = 10.5%, N(F ? 4σF) = 779, N(Var.) = 163. The compound contains to Sb2Ph4 isosteric centres [Sn2Ph4]2? as anions which are connected to rods by lithium cations in distorted tetrahedral coordination by ammonia. These rods are arranged parallel to one another in the b,c-plane, but stacked along [100].  相似文献   

14.
The First Quaternary Oxostannate with Isolated Anion Structure: RbNa3[SnO4] For the first time colourless single crystals of RbNa3SnO4 which are isotypic with NaLi3SiO4 and NaLi3GeO4 [2] have been prepared by heating e.g. a well ground mixture of RbSn and Na2O2 [Rb : Na = 1 : 4.0; 750°C; 21 d; Ni-tube]. The crystal structure was solved by four-cycle-diffractometer data [Siemens AED2; 1801 I0(hkl); space group I41/a; Z = 16; a = 1279.57, c = 1510.85 pm; R = 5.7%; Rw = 4.4%]. Mean Fictive Ionic Radii, MEFIR, Effective Coordination Numbers, ECoN, and the Madelung Part of Lattice Energy, MAPLE, are calculated. The isotypism of the compounds mentioned above is compared graphically.  相似文献   

15.
Synthesis and Structure of Tetrafluoroaurates(III) MI[AuF4] with MI = Li, Rb Single crystal investigations on Rb[AuF4], light yellow, confirm the tetragonal unit cell (K[BrF4]-type) with a = 618.2(1) and c = 1191(1) pm, Z = 4, space group I 4/mcm-D (No. 140). Li[AuF4], light yellow too, crystallizes monoclinic with a = 485.32(7), b = 634.29(8), c = 1004.43(13) pm, β = 92.759(12), Z = 4; space group P 2/c-C (No. 13). The structure of Li[AuF4] is related to the Rb[AuF4]-type of structure.  相似文献   

16.
[Li(THF)4][[NN]2Nd2Cl25-O)Li3] ( 2 ) ([NN]3– = ([Me3SiNCH2CH2)3N]3–) was prepared by transmetallation of Li3[NN] with anhydrous neodymium trichloride in THF. After recrystallization from diethylether/pentane (1 : 2) light blue crystals of 2 were obtained, which were characterized by single crystal X-ray diffraction. Space group: P21/n, Z = 4, lattice dimensions at 203 K: a = 1260.8(3), b = 3832.5(8), c = 1569.2(3) pm, β = 106.07(3)°, R1 = 0.0541. In the anion of 2 a nearly trigonal bipyramidal [Nd2Li35-O)]7+ unit is observed.  相似文献   

17.
Synthesis of Copper and Silver Complexes with Pentadentate N,S and Hexadentate N,O Chelate Ligands – Characterization and Crystal Structures of {Cu2[C6H4(SO2)NC(O)]2(C5H5N)4}, {Cu2[C5H3N(CHNC6H4SCH3)2]2}(PF6)2, and {Ag[C5H3N(CHNC6H4SCH3)2]}PO2F2 In the course of the reaction of copper(II)-acetate monohydrate with 2,2′-bisbenzo[d][1,3]thiazolidyl in methanol the organic component is transformed to N,N′-bis-(2-thiophenyl)ethanediimine and subsequently oxidized to the N,N′-bis-(2-benzenesulfonyl)ethanediaciddiamide H4BBSED, which coordinates in its deprotonated form two Cu2+ ions. Crystallisation from pyridine/n-hexane yields [Cu2(BBSED)(py)4] · MeOH. It forms triclinic crystals with the space group P1 and a = 995.5(2) pm, b = 1076.1(3) pm, c = 1120.7(2) pm, α = 104.17(1)°, β = 105.28(1)°, γ = 113.10(1)° and Z = 1. In the centrosymmetrical dinuclear complex the copper ions are coordinated in a square-pyramidal arrangement by three nitrogen and two oxygen atoms. The Jahn-Teller effect causes an elongation of the axial bond by approximately 30 pm. The reactions of the pentadentate ligand 2,6-Bis-[(2- methylthiophenyl)-2-azaethenyl]pyridine BMTEP with salts of copper(I), copper(II) and silver(I) yield the complexes [CU2(BMTEP)2](PF6)2, [Cu(BMTEP)]X2 (X = BF, C1O) and [Ag(BMTEP)]X (X = PO2F, ClO). [Cu2(BMTEP)2](PF6)2 crystallizes from acetone/diisopropyl- ether in form of monoclinic crystals with the space group C2/c, and a = 1833.2(3) pm, b = 2267.30(14) pm, c = 1323.5(2) pm, β= 118.286(5)°, and 2 = 4. In the dinuclear complex cation with the symmetry C2 the copper ions are tetrahedrally coordinated by two bridging BMTEP ligands. The Cu? Cu distance of 278.3pm can be interpreted with weak Cu? Cu interactions which also manifest itself in a temperature independent paramagnetism of 0.45 B.M. The monomeric silver complex [Ag(BMTEP)]PO2F2 crystallizes from acetone/thf in the triclinic space group P1 with a = 768.7(3) pm, b = 1074.0(5) pm, c = 1356.8(5) pm, α = 99.52(2)°, β = 96.83(2)°, γ = 99.83(2)° and Z = 2. The central silver ion is coordinated by one sulfur and three nitrogen atoms of the ligand in a planar, semicircular arrangement. The bond lengths Ag? N = 240.4–261.7 and Ag? S = 257.2 pm are significantly elongated in comparison with single bonds.  相似文献   

18.
Lithium Triamidostannate(II), Li[Sn(NH2)3] – Synthesis and Crystal Structure Rusty-red glistening, transparent crystals of Li[Sn(NH2)3] were obtained by reaction of metallic lithium with tetraphenyl tin in liquid ammonia at 110 °C. The structure was determined from X-ray single-crystal diffractometer data: Space group P 21/n, Z = 4, a = 8.0419(9) Å, b = 7.1718(8) Å, c = 8.5085(7) Å, β = 90.763(8)°, R1 (F o ≥ 4σ(F o)) = 2.8%, wR2 (F ≥ 2σ(F )) = 5.3%, N(F ≥ 2σ(F )) = 1932, N(Var.) = 65. The crystal structure contains trigonal pyramidal complex anions [Sn(NH2)3] with tin at the apex, which are connected to layers of sequence A B A B … by lithium in tetrahedra-double units [Li(NH2)2/2(NH2)2]2.  相似文献   

19.
Oxocobaltates of Alkali Metals. On Li8CoO6. Hitherto unknown Li8CoO6, rubin- red single crystals, cristallizes according to WEISSENBERG and precession photographs (MoKα) hexagonal with a = 5.44 Å, c = 10.87 Å; c/a = 2.0; Z = 2, space group C? P63cm. Atomic parameters see text. The structure derives from a closest packing of O2?, ABACA … (The tetrahedral, ?isolated”? groups [CoO4] show remarkable short distances Co–O (1.66 Å), comparable with [CoO4] in Li4CoO4, being isotypic with Li4SiO4. The MADELUNG Part of Lattice Energy is calculated and discussed.  相似文献   

20.
New Alkali Oxoarsenates(V): NaLi2[AsO4] — A New Type of Formula [1] . By heating of well ground mixtures of the binary oxides As2O3, Na2O, and Li2O2, molar ratio As:Na:Li = 1.0:1.0:2.0, in a well closed Ni tube (650°C, 21 d) colourless single crystals of NaLi2[AsO4] were obtained for the first time. The new orthoarsenate(V) crystallizes orthorhombic (space group P mn21-C, No. 31) with Z = 2. The structure determination showed that it is isostructural to βII-Li3[VO4] and that means the Li3[PO4]-type. The lattice constants a = 702.9(2) pm, b = 520.5(1) pm, c = 505.4(2) pm were taken from Guinier-Simon powder data. The structure was determined by four-circle diffractometer data [Philips PW 1 100, AgKα , 679 independent out of 2 373 Io(hkl), R = 3.03%, Rw = 2.29%; parameter see text]. The Madelung Part of Lattice Energy, MAPLE, and Effective Coordination Numbers, ECoN, these calculated via Mean Fictive Ionic Radii, MEFIR, are calculated and discussed.  相似文献   

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