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1.
New Representatives of the Er6[Si11N20]O Structure Type. High‐Temperature Synthesis and Single‐Crystal Structure Refinement of Ln(6+x/3)[Si(11–y)AlyN(20+x–y)]O(1–x+y) with Ln = Nd, Er, Yb, Dy and 0 ≤ x ≤ 3, 0 ≤ y ≤ 3 According to the general formula Ln(6+x/3)[Si(11–y)AlyN(20+x–y)]O(1–x+y) (0 ≤ x ≤ 3, 0 ≤ y ≤ 3) four nitridosilicates, namely Er6[Si11N20]O, Yb6.081[Si11N20.234]O0.757, Dy0.33Sm6[Si11N20]N, and Nd7[Si8Al3N20]O were synthesized in a radiofrequency furnace at temperatures between 1300 and 1650 °C. The homeotypic crystal structures of all four compounds were determined by single‐crystal X‐ray diffraction. The nitridosilicates are trigonal with the following lattice constants: Er6[Si11N20]O: a = 978.8(4) pm, c = 1058.8(3) pm; Yb6.081[Si11N20.243]O0.757: a = 974.9(1) pm, c = 1055.7(2) pm; Dy0.33Sm6[Si11N20]N: a = 989.8(1) pm, c = 1078.7(1) pm; Nd7[Si8Al3N20]O: a = 1004.25(9) pm, c = 1095.03(12) pm. The crystal structures were solved and refined in the space group P31c with Z = 2. The compounds contain three‐dimensional networks built up by corner sharing SiN4 and AlN4 tetrahedra, respectively. The Ln3+ and the “isolated” O2– ions are situated in the voids of the structures. According to Ln(6+x/3)[Si(11–y)AlyN(20+x–y)]O(1–x+y) an extension of the Er6[Si11N20]O structure type has been found.  相似文献   

2.
The Cluster Azides M2[Nb6Cl12(N3)6]·(H2O)4—x (M = Ca, Sr, Ba) The isotypic cluster compounds M2[Nb6Cl12(N3)6] · (H2O)4—x (M = Ca (1) , M = Sr (2) and M = Ba (3) ) have been synthesized by the reaction of an aequeous solution of Nb6Cl14 with M(N3)2. 1 , 2 and 3 crystallize in the space group Fd3¯ (No. 227) with the lattice constants a = 1990.03(23), 2015.60(12) and 2043, 64(11) pm, respectively. All compounds contain isolated 16e clusters whose terminal positions are all occupied by orientationally disordered azide ligands.  相似文献   

3.
Crystals of the chemical composition Ba7F12Cl2 were modified by adding a small amount of Ca2+ to allow the synthesis of the corresponding bromine compound Ba[Ca]7F12Br2. These samples were prepared in a NaBr flux and characterized by single crystal x‐ray diffraction. The new structure crystallizes in a disordered arrangement in the hexagonal space group P63/m (176). The calcium ion has a coordination number of 6. Solid solutions on the heavy halide position can be synthesised in a NaCl/NaBr flux to obtain the compounds Ba7?xCaxF12(ClyBr1?y)2 with x = ~0.5 and 0 < y < 1. Regardless the amount of calcium used in the preparation process, the Ca stoichiometry in the compound is always between 0.3 and 0.5. The lattice parameters differ depending on the Ca‐ and Br‐content between 1053.81(5) ? a = b ? 1058.93(3) pm and 421.21 ? c ? 426.78(3) pm.  相似文献   

4.
The Reactions of M[BF4] (M = Li, K) and (C2H5)2O·BF3 with (CH3)3SiCN. Formation of M[BFx(CN)4—x] (M = Li, K; x = 1, 2) and (CH3)3SiNCBFx(CN)3—x, (x = 0, 1) The reaction of M[BF4] (M = Li, K) with (CH3)3SiCN leads selectively, depending on the reaction time and temperature, to the mixed cyanofluoroborates M[BFx(CN)4—x] (x = 1, 2; M = Li, K). By using (C2H5)2O·BF3 the synthesis yields the compounds (CH3)3SiNCBFx(CN)3—x x = 0, 1. The products are characterized by vibrational and NMR‐spectroscopy, as well as by X‐ray diffraction of single‐crystals: Li[BF2(CN)2]·2Me3SiCN Cmc21, a = 24.0851(5), b = 12.8829(3), c = 18.9139(5) Å V = 5868.7(2) Å3, Z = 12, R1 = 4.7%; K[BF2(CN)2] P41212, a = 13.1596(3), c = 38.4183(8) Å, V = 6653.1(3) Å3, Z = 48, R1 = 2.5%; K[BF(CN)3] P1¯, a = 6.519(1), b = 7.319(1), c = 7.633(2) Å, α = 68.02(3), β = 74.70(3), γ = 89.09(3)°, V = 324.3(1) Å3, Z = 2, R1 = 3.6%; Me3SiNCBF(CN)2 Pbca, a = 9.1838(6), b = 13.3094(8), c = 16.840(1) Å, V = 2058.4(2) Å3, Z = 8, R1 = 4.4%  相似文献   

5.
The (iso)cyanurates Na[H2C3N3O3] · H2O, Na2[HC3N3O3] · H2O, Na2[HC3N3O3], and Na3[C3N3O3] were synthesized phase pure from Na2CO3 · 10H2O, NaOH, and cyanuric acid, respectively, in aqueous solution by carefully adjusting the crystallization conditions. The crystal structures of all compounds were determined by single‐crystal X‐ray diffraction {Na2[HC3N3O3] · H2O: P1 , a = 3.51660(10) Å, b = 7.8300(3) Å, c = 11.3966(4) Å, α = 86.4400(10)°, β = 85.5350(10)°, γ = 85.0720(10)°, Z = 2, R1 = 0.030, wR2 = 0.078; Na2[HC3N3O3]: Pnma, a = 6.3409(6) Å, b = 12.2382(13) Å, c = 6.5919(7) Å, Z = 4, R1 = 0.045, wR2 = 0.079; Na3[C3N3O3]: R3 c, a = 11.7459(3) Å, c = 6.5286(3) Å, Z = 3, R1 = 0.039, wR2 = 0.066}. The structures show ribbons (Na[H2C3N3O3] · H2O), dimers (Na2[HC3N3O3] · H2O), chains (Na2[HC3N3O3]), or columns (Na3[C3N3O3]) of hydrogen‐bonded and parallel stacked (iso)cyanurate anions. These motifs are shown to be characteristic for certain degrees of protonation and hydration, and all (iso)cyanurate crystal structures found so far were classified accordingly. X‐ray powder patterns, thermogravimetry curves, IR and UV/Vis spectra were measured for all compounds.  相似文献   

6.
[PtIn6][GaO4]2 – The First Oxide Containing [PtIn6] Octahedra. Preparation, Characterisation, and Rietveld Refinement – With a Remark to the Solid Solution Series [PtIn6][GaO4]2‐x[InO4]x (0 < x ≤ 1) The novel oxides [PtIn6][GaO4]2–x[InO4]x (0 < x ≤ 1) are formed by heating intimate mixtures of Pt, In, In2O3, and Ga2O3 in the corresponding stoichiometric ratio in corundum crucibles under an atmosphere of argon (1220 K, 70 h). The compounds are black, stable in air at room temperature, reveal a semiconducting behaviour, and decompose only in oxidizing acids. X‐ray powder diffraction patterns can be indexed by assuming a face centered cubic unit cell with lattice parameters ranging from a = 1001.3(1) pm (x = 0) to a = 1009.3(1) pm (x = 1). According to a Rietveld refinement [PtIn6][GaO4]2 crystallizes isotypic to the mineral Pentlandite (Fm3m, Z = 4, R(profile) = 6.11%, R(intensity) = 3.95%). The characteristic building units are isolated [PtIn6]10+ octahedra which are linked via [GaO4]5– tetrahedra to a three dimensional framework. Starting from [PtIn6][GaO4]2 the substitution of Ga3+ ions by larger In3+ ions leads to the formation of a solid solution series according to the general formula [PtIn6][GaO4]2–x[InO4]x and becomes apparent in an increase of the lattice parameter.  相似文献   

7.
Nitrido Sodalites. I Synthesis, Crystal Structure, and Properties of Zn7–xH2x [P12N24]Cl2 with 0 ? x ? 3 The nitrido sodalites Zn7–xH2x[P12N24]Cl2 with 0 ? x ? 3 are obtained by heterogeneous pressure-ammonolysis of P3N5 at presence of ZnCl2 (T = 650°C). These compounds are available too by reaction of ZnCl2, (PNCl2)3, and NH4Cl at 700°C. The crystal structures of four representatives of the above mentioned compounds have been refined by the Rietveld full-profile technique using X-ray powder diffractometer data (I4 3m, a = 821.61(4) to 824.21(1) pm, Z = 1). In the solid a three-dimensional framework of corner-sharing PN4-tetrahedra occurs (P? N: 163.6 pm, P? N? P: 125.6°, mean values) which is isosteric with the sodalite type of structure. In the center of the β-cages Cl? ions have been found, which are tetrahedrally coordinated by Zn2+ ions. The Zn2+ ions are statistically disordered. According to the phase-width observed (0 ? x ? 3) the Zn2+ ions may be partially replaced each by two hydrogen atoms which on the other hand are covalently bonded to nitrogen atoms of the P? N framework. The IR-spectra of these compounds show characteristic vibrations.  相似文献   

8.
The crystal structures of two members of the solid solution series Ag3xBi5?3xS8?6xCl6x?1 (x = 0.52 (I) , x = 0.67 (II) ) and three compounds of the Ag4xBi6?4xQ10?8xBr8x?2 series (Q = S: x = 0.70 (III) , x = 0.84 (IV) ; Q = Se: x = 0.72 (V) ) were determined by single‐crystal X‐ray diffraction. The compounds crystallize in the monoclinic space group C2/m (No. 12) with a = 1326.7(3), b = 403.9(1), c = 1176.7(2) pm, β = 107.83(3)° for (I) ; a = 1325.4(3), b = 403.3(1), c = 1170.6(2) pm, β = 108.14(3)° for (II) ; a = 1338.9(4), b = 407.7(1), c = 1426.4(4) pm, β = 113.95(2)° for (III) ; a = 1346.7(4), b = 409.3(1), c = 1440.7(4) pm, β = 114.40(1)° for (IV) ; and a = 1370.9(2), b = 417.64(4), c = 1480.4(2) pm, β = 114.92(2)° for (V) . (I) and (II) adopt the PbBi4S7 structure type, (III) to (V) crystallize in the CuBi5S8 type. All five compounds belong to the homologous series with general formula [BiQX]2[AgxBi1?xQ2?2xX2x?1]N+1 (Q = S, Se; X = Cl, Br; 1/2 ≤ x ≤ 1)), which resemble minerals of the pavonite series. They are characterized by the parameters N and x and are denoted (N, x)P. In the crystal structures, two kinds of layered modules alternate along [001]. Modules of type A uniformly consist of paired rods of face‐sharing monocapped trigonal prisms around Bi atoms with octahedra around mixed occupied metal positions (M = Ag/Bi) between them. Modules of type B are composed of chains of edge‐sharing [MZ6] octahedra (M = Ag/Bi; Z = Q/X). These NaCl‐type fragments are of thickness N = 2 in Ag3xBi5?3xS8?6xCl6x?1 and N = 3 in Ag4xBi6?4xQ10?8xBr8x?2. All structures exhibit Ag/Bi disorder in octahedrally coordinated metal positions and Q/X mixed occupation of some anion positions.  相似文献   

9.
The crystal structures of six members of the homologous series with general formula [BiQX]2[AgxBi1?xQ2?2xX2x?1]N+1 (Q = S, Se; X = Cl, Br; 1/2 ≤ x ≤ 1) and N = 4, 5, or 7 were determined by single‐crystal X‐ray diffraction. The series are characterized by the parameters N and x and are denoted (N, x)P. Ag3Bi4S6Cl3 (x = 0.60) (I) , Ag3.5Bi3.5S5Br4 (x = 0.70) (II) and Ag3.65Bi3.35Se4.70Br4.30 (x = 0.73) (III) belong to (4, x)P series Ag5xBi7?5xQ12?10xX10x?3 and adopt the AgBi6S9 structure type. The (5, x)P compound Ag3.66Bi4.34S6.68Br3.32 (IV) , which corresponds to x = 0.61 in Ag6xBi8?6xS14?12xBr12x?4, crystallizes isostructurally to AgBi3S5. The compounds Ag4.56Bi5.44Se8.88Br3.12 (x = 0.57) (V) and Ag5.14Bi4.86S7.76Br4.24 (x = 0.64) (VI) , which are members of (7, x)P series Ag8xBi10?8xQ18?16xBr16x?6, adopt the Ag3Bi7S12 structure type. In the monoclinic crystal structures (space group C2/m) two kinds of layered modules alternate along [001]. Modules of type A uniformly consist of paired rods of face‐sharing monocapped trigonal prisms around Bi atoms with octahedra around mixed occupied metal positions (M = Ag/Bi) between them. Modules of type B are composed of [MZ6] octahedra, which are arranged in NaCl‐type fragments of thickness N. All structures exhibit Ag/Bi disorder in octahedrally coordinated metal positions as well as Q/X mixed occupation of some anion positions. Corresponding to their black color, all compounds are narrow‐gap semiconductors (Eg = 0.35 eV for (II) ). General characteristics of the entire class of (N, x)P compounds are gathered in a catalogue.  相似文献   

10.
Preparation and Crystal Structures of New Complex Clorides of Lanthanides containing 3, 5‐Dimethylpyridinium Cations: (3, 5‐Dimethylpyridinium)2[LnCl4(H2O)2]Cl (Ln = La, Pr) and (3, 5‐Dimethylpyridinium)3[TbCl6] Crystals of the complex chlorides (3, 5‐dimethylpyridinium)2[LaCl4(H2O)2]Cl ( 1 ), (3, 5‐dimethylpyridinium)2[PrCl4(H2O)2]Cl ( 2 ) and (3, 5‐dimethylpyridinium)3[TbCl6] ( 3 ) have been prepared by reaction of LnCl3 · x H2O (Ln = La, Pr, Tb; x = 6‐7) with 3, 5‐dimethylpyridiniumchloride in ethanol/butanol solution. The crystal structures have been determined from single crystal X‐ray diffraction data. The compounds 1 and 2 are isotypic with each other and crystallize in the triclinic space group P1¯ (Z = 2). The 3, 5‐dimethylpyridinium cations are linked by hydrogen bonds to the anionic part of the structure built up by isolated chloride ions and strings of edge coupled triangulated dodecahedra [LnCl4/2Cl2(H2O)2]. The organic units are arranged forming a “π‐stacking”. 3 cristallizes monoclinically in the space group P21/c (Z = 4). The structure contains octahedral building units [TbCl6]3—. These octahedra are interconnected by the organic cations via hydrogen bonds forming chains parallel to [0 0 1].  相似文献   

11.
The oxonitridoaluminosilicate chloride Pr10[Si10?xAlxO9+xN17?x]Cl was obtained by the reaction of praseodymium metal, the respective chloride, AlN and Al(OH)3 with “Si(NH)2” in a radiofrequency furnace at temperatures around 1900 °C. The crystal structure was determined by single‐crystal X‐ray diffraction (Pbam, no. 55, Z = 2,a = 10.5973(8) Å, b = 11.1687(6) Å, c = 11.6179(7) Å, R1 = 0.0337). The sialon crystallizes isotypically to the oxonitridosilicate halides Ce10[Si10O9N17]Br, Nd10[Si10O9N17]Br and Nd10[Si10O9N17]Cl, which represent a new layered structure type. The structure refinement was performed utilizing an O/N‐distribution model according to Paulings rules, i.e. nitrogen was positioned on all bridging sites and mixed O/Noccupation was assumed on the terminal sites resulting in charge neutrality of the compounds. The Si and Al atoms were refined equally distributed on their three crystallographic sites, due to their poor distinguishability by X‐ray analysis. The tetrahedra layers of the structure consist of condensed [(Si,Al)N2(O,N)2] and [(Si,Al)N3(O,N)] tetrahedra of Q2 and Q3 type. The chemical composition of the compound was derived from electron probe micro analyses (EPMA).  相似文献   

12.
Preparation of Germanium-Manganese-, Germanium-Rhenium- and Tin-Rhenium-Clusters of the Type M2(CO)8[μ-EXM(CO)5]2 (M = Mn, E = Ge, X = Br, I; M = Re, E = Ge or Sn, X = I or Cl, Br, I) The clusters Re2(CO)8[μ-SnXRe(CO)5]2 are prepared by reaction of Re2(CO)10 and SnX2 in a Schlenk-tube under release of pressure (X = Cl, Br, I) or in a sealed glass tube (X = Br, I). As central structural unit a four-membered Re2Sn2 ring has to be assumed. This unit can be opened again by reaction with CO under pressure. X2Sn[Re(CO)5]2, which is also formed during the preparation of the clusters in dependance of the CO-pressure, indicates insertion of SnX2 into the Re—Re bond to be the primary step. The corresponding clusters M2(CO)8[μ-GeXM(CO)5]2 (M = Mn, X = Br, I; M = Re, X = I) are prepared by reaction of GeI2 and M2(CO)10 or of I2Ge[Mn(CO)5]2 and Mn2(CO)10 or of Br3GeMn(CO)5 and BrMn(CO)5. Ir frequencies of the new clusters are assigned.  相似文献   

13.
Solid solution phases Li7‐2xMgx[VN4] (0 < x ≤ 1) with varying Mg‐content are obtained as yellow microcrystalline powders from heat treatment of mixtures of VN, Li3N and Mg3N2 or from mixtures of Li7[VN4] and Mg3N2 at 1370 K in N2 atmosphere at ambient pressure. At substitution parameter values of x > 0.5 a subsequent distortion from the ideal cubic unit cell to an orthorhombic unit cell is observed. The crystal structure of Li7‐2xMgx[VN4] with x ≈ 1 was refined from neutron and X‐ray powder diffraction data (space group Pbca, No. 61, a = 963.03(3) pm, b = 958.44(3) pm, c = 951.93(2) pm, neutron pattern 14° — 156° 2θ, step non‐linear ≈ 0.0782° 2θ, No. of measured points 1816, Rp = 0.089, Rwp = 0.115, RBragg = 0.155, RF = 0.114; X‐ray pattern 10° — 98° 2θ, step 0.005° 2θ, No. of measured points 17600, Rp = 0.028, Rwp = 0.045, RBragg = 0.113, RF = 0.133, structure variables: 45). The crystal structure resembles a Li2O type superstructure with the atomic arrangement of β‐Li7[VN4] and with two crystallographic Li‐sites each substituted by Mg with statistical occupation factors of 0.5. Chemical analyses prove the composition and XAS spectroscopy at the V K‐edge support the +5 oxidation state assignment for vanadium. XAS data also support the tetrahedral coordination of vanadium by N as indicated by the structure refinements.  相似文献   

14.
Heteronuclear Metal Atom Clusters of the Types X4?n[SnM(CO)4P(C6H5)3]n and M2(CO)8[μ-Sn(X)M(CO)4P(C6H5)3]2 by Reaction of SnX2 with M2(CO)8[P(C6H5)3]2 (X = Halogene; M = Mn, Re; n = 2, 3) The compounds of the both types X4?n[SnM(CO)4P(C6H5)3]n (n = 3; M = Mn; X = F, Cl, Br, I. n = 2: M = Mn, Re; X = Cl, Br, I) and M2(CO)8[μ-Sn(X)M(CO)4P(C6H5)3]2 (M = Mn; X = Cl, I. M = Re; X = Cl, Br, I) are prepared by reaction of SnX2 with M2(CO)8[P(C6H5)3]2 (M = Mn, Re). Their IR frequencies are assigned. In Re2(CO)8[μ-Sn(Cl)Re(CO)4P(C6H5)3]2 the central molecule fragment contains a planar Re2Sn2 rhombus with a transannular Re? Re bond of 316.0(2) pm. Each of the SnIV atoms is connected with the terminal ligands Cl and Re(CO)4P(C6H5)3. These ligands are in transposition with respect to the Re2Sn2 ring. The mean values for the remaining bond distances (pm) are: Sn? Re = 274.0(3); Sn? Cl = 243(1), Re? C = 176(5), Re? P = 242.4(9), C? O = 123(5). The factors with an influence on the geometrical shape of such M2Sn2 rings (M = transition metal) are discussed.  相似文献   

15.
Studies on Polypseudohalides. 4. Preparation and Crystal Structure of KxRb1?x[I(CN)2] · 1/2 C6H12N2O2 (x = 0.6) The new compound KxRb1?x[I(CN)2] · 1/2 C6H12N2O2 (x = 0.6), C10H12I2K1·2N6O2Rb0·8, may be prepared by the addition of rubidium bromide to a saturated solution of iodine cyanide and potassium cyanide in a mixture of ethanol and water. Potassium bromide and rubidium bromide are formed as by-products. The compound has been investigated by chemical analysis, spectroscopy and structural analysis based on single crystal X-ray data. At room temperature it crystallizes in the monoclinic space group P21/c with a = 436.34 pm, b = 1933.5 pm, c = 1240.5 pm, β = 92.30° and Z = 4. The compound may be described as a solvated salt which is built up by a cation statistically occupied with potassium and rubidium and the trihalide-analogous anion [I(CN)2]?. Additional there is one molecule Diimino-oxalic-acid-di-ethyl-ester per two formula units M[I(CN)2]. The asymmetricanion is nearly linear. The bond lengths d(I? C) = 226.5 pm, 235.1 pm are extended compared with the analogous distance in iodine cyanide. The surrounding of the cation is a distorted octahedron. The structure of the solvating molecule is quite normal. The crystal structure may be interpreted as a sequence of puckered ionic layers paralledl to (001) which are connected through the cations. The organic molecules are intercalated in channels along [100] between these layers.  相似文献   

16.
Alkali Metal Nitrido Tecto Metallates(VI) with Networks of Six‐membered Rings of Corner‐sharing Tetrahedra [(MNN3/2)6] with M = Mo, W of the Unexpected Composition A9+x[M6N15] with A = Rb, Cs and 0 < x < 1 Reactions of metal powders of Mo and W respectively with amides and azides of Rb and Cs lead to the compounds Rb9+x[W6N15] and Cs9+x[M6N15] with M = Mo, W and 0 < x < 1. The reactions are carried out at 650 °C in autoclaves for salt melts and are finished within 5 d. Crystals of the compounds are embedded in a matrix of the corresponding alkali metal. These metals result from the thermal decomposition of the amides and azides used in high molar ratios. The metals are washed out by liquid ammonia. Besides microcrystalline material of the above mentioned compounds single crystals suitable in size for x‐ray structure determinations were isolated. The compounds crystallize in the space group R3c (No. 167) with Z = 6 and the following lattice constants: Rb9+x[W6N15]: a = 12.743(7) Å, c = 27.794(8) Å, c/a = 2.181 Cs9+x[Mo6N15]: a = 13.104(5) Å, c = 28.430(9) Å, c/a = 2.170 Cs9+x[W6N15]: a = 13.136(5) Å, c = 28.472(6) Å, c/a = 2.167 The metal centres of tetrahedra [MNN3/2] are condensated to cyclohexane analogue six‐membered rings in chair‐form via nitrogen atoms and axial ones connect them to a three‐dimensional network. Nine – as to the formula unit – of the alkali metal atoms are located in vacancies of the anionic partial structure. The residual atoms with 0 < x < 1 centre the six‐membered rings and are coordinated planar hexagonal by N neighbours.  相似文献   

17.
Reduction of tin disulfide SnS2 leads in a reversible topotactic reaction to the formation of layered hydrated phases A x + (H2O)y[SnS2]x–. The latter exhibit polyelectrolyte character, i. e. ion exchange and solvent exchange reactions as a consequence of the high mobility of the interlayer species. Structure and properties of the tin sulfide hydrates are closely related to those of transition metal dichalcogenide hydrates.
Topotaktische Bildung und Austauschreaktionen von hydratisierten Zinnsulfiden Ax(H2O)ySnS2 mit Schichtstruktur
Zusammenfassung Die Reduktion von Zinndisulfid führt in einer reversiblen topotaktischen Reaktion zur Ausbildung von hydratisierten Phasen A x + (H2O)y[SnS2]x– mit Schichtengitterstruktur. Diese weisen Polyelektrolytcharakter auf, d.h. sie zeigen Ionenaustausch- und Lösungsmittelaustausch-Reaktionen als eine Folge der großen Beweglichkeit der Moleküle zwischen den Schichten. Struktur und Eigenschaften der Zinnsulfid-Hydrate stehen denen der Übergangsmetalldichalkogenid-Hydrate sehr nahe.
  相似文献   

18.
Preparation of trans-[Pt(N3)4X2]2? (X ? Br, I, SCN, SeCN) by Oxidative Addition to [Pt(N3)4]2? in Organic Solvents By oxidative addition to (TBA)2[Pt(N3)4], dissolved in dichlormethane, trans-(TBA)2[Pt(N3)4X2], X ? Br, I, SCN, SeCN; TBA = Tetrabutylammonium, are formed. The vibrational spectra of these salts are assigned according to point group D4h. From the resonance Raman spectrum of trans-(TBA)2[Pt(N3)4I2] the harmonic vibrational frequency ω1 of v(Pt? I), A1g, is calculated to be 138.50 cm?1 and the inharmonicity constant x11 = 0.27 cm?1. The characteristical feature in the UV/VIS spectra is caused by intensive π(N,X) → a1g, b1g(Pt) CT transitions.  相似文献   

19.
The phase and chemical compositions of the precipitates formed in the LiVO3-VOSO4-H2O system at initial pH within 1 ≤ pH ≤ 4 and 90°C were studied. The following phases were prepared: an α phase Li1.4(VO)1.3[H2V10O28] · nH2O and a β phase Li0.6 ? x H1.4 + x [V12O31 ? y/2] · nH2O (0 ≤ x ≤ 0.5, 1.3 ≤ y ≤ 2.0) with a layered structure. Li0.4V2O5 · H2O nanorods with the interlayer distance 10.30 ± 0.08 Å were synthesized at 180°C in an autoclave. The morphology, IR spectra, and main formation processes for these polyvanadates were studied.  相似文献   

20.
The local structure of the double perovskite (Sr2‐xCax)FeMoO6 (0 ≤ × ≤ 2.0) and Sr2CrMO6 (M = Mo, W) systems have been probed by extended X‐ray absorption fine structure (EXAFS) spectroscopy at the Fe and Cr K‐edges. We found Fe‐O (ave) distance apparently decreases from 1.999 Å (x = 0) to 1.991 Å (x = 1.0) in (Sr2‐xCax)FeMoO6 (tetragonal structure). When x is increased further from 1.5 to 2.0, the Fe‐O bond distance decreased from 2.034 Å to 2.012 Å (monoclinic structure). In addition, Cr‐O, Sr‐Cr, and Cr‐Mo bond distances in Sr2CrWO6 are all slightly larger than the bond distances of Sr2CrMoO6, which is due to the ionic radius of the W5+ (0.62 Å) which is larger than the ionic radius of Mo5+ (0.61 Å). The results are consistent with our XRD refinements data.  相似文献   

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