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Synthesis, Structure, and Magnetic Properties of Compounds NaMIIZr2F11 (MII = Ti, V, Cu) and a Notice on NaPdZr2F11 By synthesizing NaTiZr2F11 in form of red single crystals, it was possible to obtain a complex fluoride with Ti2+ for the first time. It crystallizes like the analogous greenish blue vanadium compound isotypic to AgPdZr2F11 [1] monoclinic, spacegroup C2/m–C (No. 12) with a = 918.0/911.5 pm, b = 682.6/675.7 pm, c = 780.8/776.6 pm, β = 116.2/116.2º and Z = 2. Colourless NaCuZr2F11 however crystallizes as a result of the Jahn-Teller distortion of Cu2+ triclinic (space group P1 –C (No. 2), a = 552.7 pm, b = 568.2 pm, c = 768.0 pm, α = 111.0º, β = 97.4º, γ = 106.4º) and is – as expected – isotypic to NaAgZr2F11 [1].  相似文献   

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The Crystal Structures of the Vanadium Weberites Na2MIIVIIIF7 (MII ? Mn, Ni, Cu) and of NaVF4 At single crystals of the vanadium(III) compounds NaVF4 (a = 790.1, b = 531.7, c = 754.0 pm, β = 101.7°; P21/c, Z = 4), Na2NiVF7 (a = 726.0, b = 1031.9, c = 744.6 pm; Imma, Z = 4) and Na2CuVF7 (a = 717.6, b = 1043.5, c = 754.6 pm; Pmnb, Z = 4) X-ray structure determinations were performed, at Na2MnVF7 (a = 746.7, c = 1821.6 pm; P3221, Z = 6) a new refinement. NaVF4 crystallizes in the layer structure type of NaNbO2F2. The fluorides Na2MIIVF7 represent new orthorhombic (MII ? Ni; Cu) resp. trigonal (MII ? Mn) weberites. The average distances within the [VF6] octahedra of the four compounds are in good agreement with each other and with data of related fluorides (V? F: 193.3 pm). The differences between mean bond lengths of terminal and bridging F ligands are 5% in NaVF4, but less than 1% in the weberites. Details and data for comparison are discussed.  相似文献   

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Synthesis and Crystal Structure of Manganese(II) and Zinc Amides, Mn(NH2)2 and Zn(NH2)2 Metal powders of manganese resp. zinc react with supercritical ammonia in autoclaves in the presence of a mineralizer Na2Mn(NH2)4 resp. Na2Zn(NH2)4_.0.5NH3 to well crystallized ruby‐red Mn(NH2)2 (p(NH3) = 100 bar, T = 130°C, 10 d) resp. colourless Zn(NH2)2 (p(NH3) = 3.8 kbar, T = 250°C, 60 d). The structures including all H‐positions were solved by x‐ray single crystal data: Mn(NH2)2: I41/acd, Z = 32, a = 10.185(6) Å, c = 20.349(7) Å, N(Fo) with F > 3σ (F) = 313, N(parameter) = 45, R/Rw = 0.038/0.043. Zn(NH2)2: I41/acd, Z = 32, a = 9.973(3) Å, c = 19.644(5) Å, N(Fo) with F > 3σ (F) = 489, N(parameter) = 45, R/Rw = 0.038/0.043. Both compounds crystallize isotypic with Mg(NH2)2 [1] resp. Be(NH2)2 [2]. Nitrogen of the amide ions is distorted cubic close packed. One quarter of tetrahedral voids is occupied by Mn2+‐ resp. Zn2+‐ions in such an ordered way that units M4(NH2)6(NH2)4/2 occur. The H‐atoms of the anions have such an orientation that the distance to neighboured cations is optimum.  相似文献   

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Jahn-Teller Distortions of Transition Metal Ions in Tetrahedral Coordination — The Structures of Cat[MII(NCS)4]II (MII: Co, Ni, Cu) and of Mixed Crystals MIICr2O4(MII: Zn? Ni, Zn? Cu, Cu? Ni) of the Spinel Type The structure determination of compounds Cat[MII(NCS)4] with Cat = p-xylylenebis(triphenylphosphonium)2+ and MII = Co, Ni, Cu [space group P21/n, Z = 4] yielded pseudotetrahedral MIIN4-polyhedra, which are distorted by packing forces and vibronic coupling effects of the Jahn-Teller type. Spinel mixed crystals with MII = Zn? Ni, Zn? Cu, Ni? Cu in the tetrahedral sites exhibit phase transition to tetragonal and o-rhombic structures, induced by cooperative Jahn-Teller interactions. The distortion symmetries of the MIIN4 and MIIO4 tetrahedra are analysed on the basis of the respective electronic groundstate and the possible Jahn-Teller active vibrational modes.  相似文献   

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[CrIII8MII6]12+ (MII=Cu, Co) coordination cubes were constructed from a simple [CrIIIL3] metalloligand and a “naked” MII salt. The flexibility in the design proffers the potential to tune the physical properties, as all the constituent parts of the cage can be changed without structural alteration. Computational techniques (known in theoretical nuclear physics as statistical spectroscopy) in tandem with EPR spectroscopy are used to interpret the magnetic behavior.  相似文献   

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Zusammenfassung In den beiden untersuchten Doppelfluorid-Serien, BaMF4 und Pb2 MF6 (M=Mn, Fe, Co, Ni, Cu, Zn), zeigen die Verbindungen des Cu und des Zn ein anderes Verhalten als die übrigen. Die Zn-Verbindungen sind diamagnetisch, die Cu-Verbindungen paramagnetisch. Pb2CuF6 befolgt dasCuriesche Gesetz, während BaCuF4 eineCurie-Weiss-Abweichung unterhalb 212 K aufweist.Im untersuchten Temperaturbereich zeigt sich für alle anderen Verbindungen, mit Ausnahme von Pb2FeF6, Antiferromagnetismus.
Magnetic properties of the compounds BaMF4 and Pb2 MF6 (M=Mn, Fe, Co, Ni, Cu, Zn)
Two series of double fluorides, BaMF4 and Pb2 MF6 (M=Mn, Fe, Co, Ni, Cu, Zn) have been studied, the compounds of Cu and Zn differing in behaviour from the others. The Zn componds are diamagnetic, the Cu compounds paramagnetic. Pb2CuF6 conforms toCurie's law while BaCuF4 exhibits aCurie-Weiss deviation below 212° K.With the exception of Pb2FeF6, all the other compounds show antiferromagnetism in the studied temperature range.


Mit 5 Abbildungen

Herrn Prof. Dr.Hans Nowotny ergebenst gewidmet.  相似文献   

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Mg2(PO2NH)4 · 8 H2O ( 1 ), Mn2(PO2NH)4 · 8 H2O ( 2 ), Co2(PO2NH)4 · 8 H2O ( 3 ) and Zn2(PO2NH)4 · 8 H2O ( 4 ) were obtained as microcrystalline powders by combining aqueous solutions of K4(PO2NH)4 · 4 H2O and MX2 · y H2O (M = Mg, Mn, Co, Zn; X = Cl, NO3). Single crystals were obtained by crystallization in gelatine gels in U‐tubes or test‐tubes. 2 and 4 were characterized by thermogravimetry and 4 was additionally characterized by temperature dependend in situ powder diffractometry. The structures of 1 , 2 , 3 and 4 were found to be isotypic and were solved by single‐crystal X‐ray methods: P 21/c, Z = 2 ( 1 : a = 645.4(2), b = 1050.1(2), c = 1283.3(3) pm, β = 104.66(3)°; 2 : a = 648.7(2), b = 1063.1(2), c = 1310.8(3) pm, β = 103.93(3)°; 3 : a = 643.3(2), b = 1049.0(2), c = 1286.7(3) pm, β = 104.28(3)°; 4 : a = 644.18(5), b = 1049.22(7), c = 1282.43(8) pm, β = 104.122(6)°). The structure is composed of MO6 octahedra and (PO2NH)44— anions. The P4N4 rings of the (PO2NH)44— anions exhibit a slightly distorted chair conformation, which is supported by IR data and has been described by torsion angles, Displacement Asymmetry Parameters and Puckering Parameters. Via M2+ ions and hydrogen bonds, the tetrametaphosphimate anions are connected forming layers perpendicular to [100]. These layers are connected by hydrogen bonds.  相似文献   

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New Syntheses and Crystal Structures of Bis(fluorophenyl) Mercury, Hg(Rf)2 (Rf = C6F5, 2, 3, 4, 6‐F4C6H, 2, 3, 5, 6‐F4C6H, 2, 4, 6‐F3C6H2, 2, 6‐F2C6H3) Bis(fluorophenyl) mercury compounds, Hg(Rf)2 (Rf = C6F5, C6HF4, C6H2F3, C6H3F2), are prepared in good yields by the reactions of HgF2 with Me3SiRf. The crystal structures of Hg(2, 3, 4, 6‐F4C6H)2 (monoclinic, P21/n), Hg(2, 3, 5, 6‐F4C6H)2 (monoclinic, C2/m), Hg(2, 4, 6‐F3C6H2)2 (monoclinic, P21/c) and Hg(2, 6‐F2C6H3)2 (triclinic, P1) are described.  相似文献   

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Structure and Magnetism of Fluorides Cs2MCu3F10 (M = Mg, Mn, Co, Ni), Variants of the CsCu2F5 Type X‐ray structure determinations of single crystals showed that compounds Cs2MCu3F10 crystallize with Z = 2 in space group P21/n (No.14) (M = Mn) of the CsCu2F5 type resp. in its supergroup I2/m (No.12) (M = Mg, Co, Ni). Cs2MgCu3F10: a = 714.9(1), b = 736.8(1), c = 940.4(1) pm, b = 96.29(1)°, (Mg‐F: 199.2 pm); Cs2MnCu3F10: a = 725.1(1), b = 742.7(1), c = 951.0(2) pm, b = 97.28(3)°, (Mn‐F: 209.1 pm); Cs2CoCu3F10: a = 717.8(3), b = 739.1(2), c = 939.4(4) pm, b = 97.49(2)°, (Co‐F: 203.1 pm); Cs2NiCu3F10: a = 716.3(1), b = 737.7(1), c = 938.2(2) pm, b = 97.09(1)°, (Ni‐F: 201.0 pm). As determined directly for the Mg compound and generally concluded from the average distances M‐F noted, M substitution concerns mainly the octahedrally coordinated position of the CsCu2F5 structure, the distortion of which is very much reduced thereby. Within the remaining [CuF4] and [CuF5] coordinations, in contrast to CsCu2F5, one F ligand is disordered, in case of the Mn compound the pyramidally coordinated Cu atom, too. The magnetic properties are complex and point to frustration and spin glass effects. Only at the diamagnetically substituted variants with M = Mg, Zn no Néel point appears, which is reached at 27, 23, 36 and 55 K for M = Mn, Co, Ni and Cu, resp. At lower temperatures ferri‐ resp. weak ferromagnetism and hysteresis is observed.  相似文献   

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Synthesis and Crystal Structure of Sr2Zn(OH)6 and Ba2Zn(OH)6 Crystallization from supersaturated sodium hydroxozincate solutions by adding solutions of alkali earth metal hydroxides yields crystals of Sr2Zn(OH)6 and Ba2Zn(OH)6. The X-ray structure determination on these crystals was successful including all hydrogen positions: Sr2Zn(OH)6: P21/n, Z = 2, a = 5.794(1) Å, b = 6.160(1) Å, c = 8.141(1) Å, b = 91.23(1)°, N(F ³° 2σ F) = 1127, N(Var.) = 53, R1/wR2 = 0.047/0.081Ba2Zn(OH)6: P21/n, Z = 2, a = 6.043(1) Å, b = 6.336(1) Å, c = 8.451(2) Å, b = 91.23(2)°, N(F ° 2σ F) = 1669, N(Var.) = 54, R1/wR2 = 0.029/0.067. Sr2Zn(OH)6 and Ba2Zn(OH)6 crystallize isotypic in a distorted Li2O structure type. Sr2+ resp. Ba2+ form a cubic primitive arrangement. Distorted octahedra of OH around Zn2+ fill therein alternating cubic gaps in an ordered way.  相似文献   

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Phosphoraneiminato Acetate Cluster of Copper and Zinc. Crystal Structures of [Cu4(NPEt3)2(O2CCH3)6] and [Zn4(NPEt3)2(O2CCH3)6] The anhydrous acetates of copper(II) and zinc react with the silylated phosphaneimine Me3SiNPEt3 in dichloromethane at 20 °C forming the mixed phosphoraneiminato acetate clusters [Cu4(NPEt3)2(O2CCH3)6] ( 1 ), which forms emerald crystals, and colourless [Zn4(NPEt3)2 · (O2CCH3)6] ( 2 ). In spite of analogous composition the structures of 1 and 2 are completely different. In the asymmetric unit of 1 three copper atoms of an almost isosceles triangle are linked via two nitrogen atoms of the NPEt3 groups to form a trigonal bipyramidal aggregate. One of these three copper atoms is chelated by an acetate group, another one is connected with the fourth copper atom via three μ2‐O2C–CH3 groups. The asymmetric units are associated via a μ2‐O2C–CH3 group and a μ3‐OC(O)CH3 group at a time so that infinite chains result. In 2 two zinc atoms are linked via the nitrogen atoms of the two NPEt3 groups to form an almost centrosymmetric four‐membered ring. Both nitrogen atoms of the four‐membered ring are connected with another zinc atom each. These zinc atoms again are linked with the zinc atoms of the Zn2N2 four‐membered ring via two μ2‐O2C–CH3 groups each and additionally coordinated with a terminal acetate ligand each.  相似文献   

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Synthesis and Structure of MII[AuF4]2 (MII ? Cd, Hg) Cd[AuF4]2 and the isotypic compound Hg[AuF4]2, both are yellow, crystallize tetragonal in the space-group P4/mcc-D (No. 124) with a = 575.0/575.6 pm, c = 1034.8/1042.3 pm and Z = 2. The single-crystals were obtained by solid-state reactions in goldtubes.  相似文献   

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Syntheses and Properties of Di‐tert‐butylphosphides [M(PtBu2)2]2 (M = Zn, Hg) and [Cu(PtBu2)]4 The phosphides [M(PtBu2)2]2 (M = Zn, Hg) and [Cu(PtBu2)]4 are accessible from reaction of LiPtBu2 with ZnI2, HgCl2 and CuCl, respectively. [M(PtBu2)2]2 (M = Zn, Hg) are dimers in the solid state. X‐ray structural analyses of these phosphides reveal that [M(PtBu2)2]2 (M = Zn, Hg) contain four‐membered M2P2‐rings whereas [Cu(PtBu2)]4 features a planar eight‐membered Cu4P4‐ring. Degradation reaction of LiPtBu2(BH3) in the presence of HgCl2 results in the dimeric phosphanylborane BH3 adduct [tBu2PBH2(BH3)]2. X‐ray quality crystals of [tBu2PBH2(BH3)]2 (monoclinic, P21/n) are obtained from a pentane solution at 6 °C. According to the result of the X‐ray structural analysis, the O2‐oxidation product of [Hg(PtBu2)2]2, [Hg{OP(O)(tBu)OPtBu2}(μ‐OPtBu)]2, features in the solid state structure two five‐membered HgP2O2‐rings and a six‐membered Hg2P2O2‐ring. Herein the spiro‐connected Hg atoms are member of one five‐membered and of the six‐membered ring.  相似文献   

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New Complex Fluorides with Ag2+ and Pd2+: NaMIIZr2F11 (MII = Ag, Pd) and AgPdZr2F11 For the first time single crystals of NaAgZr2F11, NaPdZr2F11 and AgPdZr2F11 have been obtained and investigated by X-ray methods. The isotypic compounds NaMIIZr2F11 (MII = Ag, Pd) crystallize triclinic, spcgr. P1 ? C (No. 2) with a = 780.9, b = 570.0, c = 583.2 pm, α = 106.1°, β = 112.2°, γ = 97.9° (NaPdZr2F11), AgPdZr2F11 is monoclinic, spcgr. C2/m? C2h (No. 12) with a = 935.1, b = 699.1, c = 780.1 pm, β = 115.7°, Z = 2 (Four circle diffractometer data, Siemens AED 2). Their structure is closeley related to the Ag3Hf2F14-type of structure.  相似文献   

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