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1.
X-Ray and Vibrational Studies of Sulvanite Mixed Cystals Cu3Nb(SxSe1?x)4, Cu3Nb(SexTe1?x)4, Cu3Ta(SxSe1?x)4 and Cu3Ta(SexTe1?x)4 Solid solutions Cu3Nb(SxSe1?x)4, Cu3Nb(SexTe1?x)4, Cu3Ta(SxSe1?x)4 and Cu3Ta(SexTe1?x)4 with sulvanite structure have been prepared in the range 0 ≤ x ≤ 1. The lattice constants in all systems obey the Vegard rule. Infrared and Raman spectra have been measured. The spectra of the compounds with mixed anion sublattices show additional peaks, compared to those of the end members, because besides the polyhedra MX4 and MY4 also groups MX3Y, MX2Y2, and MXY3 are present, and all groups are able to oscillate independently. By comparison of the peak intensities and the statistical frequency of the groups according to the composition, the additional valence vibrations could be attributed to the groups.  相似文献   

2.
Three new series of mixed-ligand clusters of the [(M6X12)X2(RCN)4] (M=Nb, Ta; X=Cl, Br; R=Et, n-Pr, n-Bu) composition have been prepared. It is supposed that four nitrile molecules and two halogen atoms are coordinated to the terminal octahedral coordination sites of the [M6X12]2+ unit.  相似文献   

3.
Contributions to the Chemistry of Niobium and Tantalum. 88. Cluster Hydroxides [M6X12](OH)2 · 8 H2O with M = Nb, Ta; X = Cl, Br The cluster hydroxides [M6X12](OH)2 · 8 H2O with M = Nb, Ta; X = Cl, Br, have been prepared. The poor crystalline compounds could not be classified in any of the four general structure patterns of the niobium and tantalum halide compounds. Infrared spectra, magnetic and thermal behaviours of the compounds have been measured and discussed.  相似文献   

4.
A detailed investigation on the new series of compounds(MX4)nY (M =Nb, Ta; X =S, Se; Y =Br, I)is given through structural information and resistivity measurements. All these compounds are built with the same framework which is composed ofMX4chains and halogen atoms between these chains. It is found that the resistivity behavior is closely related to the metal-metal sequence along theMX4chain.  相似文献   

5.
On Compounds of the Type Cu3MSxSe4?x(M = Nb, Ta). Determination of Crystal Structure of Cu3TaSSe3 The preparation, X-ray data, vibrational, and electronic spectra of Cu3NbS3Se, Cu3NbS2Se2, Cu3NbSSe3, Cu3TaS3Se, Cu3TaS2Se2, and Cu3TaSSe3 are reported. The powder patterns of all compounds could be indexed on the basis of a simple cubic lattice. The compounds crystallize in pseudo-sulvanite type with the sulfur and selenium atoms in random distribution.  相似文献   

6.
Syntheses and Crystal Structures of the Phases 6R? CuxM1+yS2 (M = Nb, Ta) Thermal decomposition of 2H? Cu0.66MS2 (M = Nb, Ta) results in the formation of 6R? CuxM1+yS2. Crystals can be obtained by chemical vapour transport reactions with iodine in a temperature gradient (1320–1220 K). The structures of four phases with trigonal symmetry (R3 m, Z = 6) were determined from single crystal x-ray diffraction data. Nb and Ta, resp., of the MS2 partial structures have a trigonal prismatic coordination. The additional metal atoms are distributed at random only in S-octahedra (Nb, Ta) and -tetrahedra Cu sharing faces with MS6-prisms. The sequence of the layers can be rationalized on the assumption of stabilizing interactions between metal atoms in adjacent layers.  相似文献   

7.
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   

8.
Bismuth(II) Chalcogenometallates(III) Bi2M4X8, Compounds with Bi24+ Dumbbells (M = Al, Ga and X = S, Se) The ternary bismuth(II) chalcogenometallates(III) Bi2M4X8 (with M = Al, Ga and X = S, Se) were synthesized from the binary chalcogenides M2X3 and Bi2X3 and elementary bismuth. All compounds are diamagnetic semiconductors with Eg (opt.) = 1.8–2.7 eV. The phases (except Bi2Al4Se8) are thermodynamically stable and decompose peritectically above 965–1020 K. Bi2Al4Se8 is metastable below 825 K and is obtained only by rapid quenching from T > 825 K. The isotypic compounds crystallize in a new tetragonal tP28 structure type (P4/nnc). The characteristic unit is the hitherto unknown clustercation Bi24+, with the mean bond length d(Bi–Bi) = 314.2 pm, the Raman frequency 102 cm–1 ≤ νs ≤ 108 cm–1, and the mean force constant of f = 0.68 N · cm–1. The Electron Localization Function, ELF, shows the covalent Bi–Bi bond, the lone electron pairs of the ψ-octahedrally coordinated Bi(II) cations, and the polar character of the Bi–X bonds.  相似文献   

9.
The products of the high temperature reaction of Ta2S with equimolar amounts of V and Cr, respectively, have been characterized by X-ray spectrometry and diffraction. The structures of the metal-rich compounds MxTa6?xS (M = V, Cr; x ? 1) have been determined from with single crystal X-ray intensities. The isotypic phases crystallize in the monoclinic space group C2/c four formula units per unit cell. The structure is interpreted as consisting of interpenetrating distorted metal icosahedra arranged to columns which in turn are connected to form layers via additional Ta? Ta interactions. Metal-sulphur and weaker metal–metal Bonds provide the linkage of the layers. The coordination about S is square antiprismatic. The structural relationship and fundamental distinctions between MxTa6?xS and Ta6S are pointed out. Thermodynamic quantities are used to elucidate the various reaction products and differences between Ta6?xVxS and CrxTa6?xS with respect to the phase widths.  相似文献   

10.
Nitrido-Sodalites. II. Synthesis, Crystal Structure, and Properties of M(6+(y/2)–x)H2x[P12N24]Zy with M = Fe, Co, Ni, Mn; Z = Cl, Br, I; 0 ≤ x ≤ 4; y ≤ 2 The nitrido sodalites M(6+(y/2)–x)H2x[P12N24]Zy with M = Fe, Co, Ni, Mn; Z = Cl, Br, I; 0 ≤ x ≤ 4; y ≤ 2 are obtained by the reaction of HPN2 or [PN(NH2)2]3 with the metal halogenide MZ2 (T = 700°C). The compounds are isotypic to Zn(7–x)H2x[P12N24]Cl2. An increase of the ionic radii of the cations or anions results in an expansion of the lattice which is caused by an increase of the P? N? P angle. The influence of the cation is more dominant than that of the anion. By reacting [PN(NH2)2]3 with metal halogenide (MZ2) hydrogen free, X-ray amorphous products are obtained. The formation of the chloride-containing P? N-sodalite in this reaction begins at temperatures below 450°C.  相似文献   

11.
Spinels with substituted Nonmetal Sublattices. IV. CuCr2(S1?xSex)4 and CuCr2(Se1?xTex)4 Polycrystalline samples of the spinel system CuCr2(S1?xSex)4 have been prepared with 0 ≤ x ≤ 1. We found that in the spinel system CuCr2(Se1?xTex)4 no solid solution is existent in the range 0.01 ≤ x ≤ 0.70. When S is substituted by Se and Se by Te the lattice constants increase linearely by 0.52 Å and 0.81 Å respectively. The anion-sublattice shows random distribution of the chalcogen atoms, the chalcogen parameters u are constant in the system CuCr2(S1?xSex)4 with a mean value of u = 0.3829. The calculated anion-cation-distances lead to a covalent tetrahedral radius rCu = 1.23 Å. This radius is in agreement with the radius rCu = 1.22 Å of Cu spinels with Cu in the valence +1.  相似文献   

12.
Entry to the Chemistry of Simple Rhenium Sulfur Complexes and Clusters. Preparation and Crystal Structures of R′[ReS4], R′[ReS9], (NH4)4[Re4S22]·2H2O, R′2[Cl2Fe(MoS4)FeCl2]1-x, R′2[(ReS4)Cu3I4] and RR′2[(ReS4)Cu5Br7] (R ? NEt4; R′ ? PPh4, x = 0.3, 0.5) The compounds R[ReS4] ( 1 ), R′[ReS9] ( 2 ), (NH4)4[Re4S22]·2 H2O ( 3 ), R′2[Cl2Fe(MoS4) FeCl2]x[Cl2Fe(ReS4)FeCl2] 1-x (x = 0.3 ( 4 ), 0.5), R′2[(ReS4)Cu3I4] ( 5 ) and R′2[(ReS4)Cu5Br7] ( 6 ) (R ? NEt4; R′ ? PPh4) have been prepared by reaction of perrhenates or rhenium(VII)oxide with Sx2? solutions (under different conditions) or by reactions of metal-halides with [ReS4]?-ions. All compounds have been characterized by complete X- ray structure analysis. For further details see Inhaltsübersicht.  相似文献   

13.
X-ray diffraction patterns for the cluster compounds [M6X12i]X2a · nH2O, M = Nb, Ta; Xi = Cl, Br; Xa = Cl, Br, I, OH (i — inside, a — outside) have been measured and compared, according to which cluster hydroxides [M6Br12](OH)2 · 8 H2O can be classified in the previously known structural group B. Analogous chloro-cluster hydroxides form a separate structural group E.  相似文献   

14.
In this study, Fe x Ti1–2x M x O2 (M=Nb, Ta) rutile solid solutions have been synthesized from gels made from Fe(III) acetylacetonate, NbCl5, TaCl5, Ta(V) ethoxide, TiCl4 and Ti(IV) isopropoxide. The results obtained are compared with those obtained by the ceramic method. The solid solutions synthesized from gels were obtained at lower temperatures than these synthesized by the ceramic method.  相似文献   

15.
Electrochemical Reduction of CSSe and CSe2 in Dimethylformamide: Heterocyclic 1,2-Dichalcogenolates and their Coordination Chemistry Starting from carbon diselenide or carbon selenidesulfide the electrochemical preparation (electrosynthesis) of heterocyclic dichalcogenolates C3X52? (X = Se: dsis; X = S/Se: C3SxSey2?) is outlined. The 1,2-dichalcogenolate compounds were isolated and characterized as dibenzoyl derivatives. Bis- or tris-chelates of general type Am[M(C3X5)n] (with A = Bu4N+, Ph4As+; M = ZnII, PtII, PdII, NiIII, CuIII, AuIII, InIII; X = Se, S/Se; m = 1, 2, 3; n = 2, 3, respectively) are available directly from methanolic solutions of the dibenzoylates after hydrolytic cleavage of the latter with sodium methanolate. In addition bis-chelates Bu4N[Ni(C3X5)2] (X = Se, S/Se) have been characterized by cyclovoltammetry and epr spectroscopy and compared with the corresponding all-sulfur ligand compound Bu4N[Ni(dmit)2] (X = S). Arguments are given for the fact that the allselenium ligand dsis (X = Se) yields the CuIII or NiIII chelate at once whereas with dmit using identical conditions the metal(II) compounds are formed.  相似文献   

16.
Synthesis, Structure, and Properties of the Tetraarsenidometallates(V) M7[TAs4] (M = K, Rb; T = Nb, Ta) The tetraarsenidometallates(V) M7[TAs4] (M = K, Rb; T = Nb, Ta) have been prepared from RbAs, KAs, Rb3As, K3As, and Nb or Ta in sealed Nb(Ta) ampoules at T = 1100 K. They crystallize in a new structure type oP24 (Pmn21, no. 31); K7[NbAs4]: a = 1019.2(2) pm, b = 916.2(2) pm, c = 830.6(1) pm; K7[TaAs4]: a = 1017.3(2) pm, b = 915.5(2) pm, c = 830.5(2) pm; Rb7[NbAs4]: a = 1059.2(4) pm, b = 952.8(4) pm, c = 860.4(4) pm; Z = 2 formula units per unit cell). The compounds form dark red crystals and they are sensitive against air and moisture. They are semiconductors with Eg = 1.80 eV. The thermal decomposition in dynamical vacuum gives evidence for the existance of K4TAs3 and K2TAs2 (T = Nb, Ta). Main structural units are polar oriented tetrahedra [TAs4] with d (T – As) = 252.2(1) pm; 251.3(1) pm; 253.0(4) pm, respectively. The As atoms are trigonal prismatically coordinated by M and T atoms. These trigonal prisms form anionic and cationic layers [M4As2]2? and 2[M3TAs2]2+ alternating along the b axis. The structure is comparable with that of Co2P and can be described as a stuffed shear variant of the Na6□ZnO4 type of structure.  相似文献   

17.
Abstract

Some binary cyclo-tetraphosphates have been synthetized by means of thermal dehydration of the starting binary dihydrogenphosphate. The mechanism of dehydration and condensation reactions in dependence on various special conditions of thermal preparation (temp. rate, water vapour pressure, using nuclei) has been studied. The methods of TA at quasi-isothermal and quasi-isobaric conditions with combination of calcination experiments have been used for these purposes. The reaction products obtained were analyzed by chromatography, IR-spectrosco-py, X-ray diffraction analysis, electron microscopy and AAS. The course, the rate and the yields of the condensation reactions of formation of the main products considered Cu2-xMgxP4O12 and Ni2-xMgXP4)12, have been investigated. These coloured products (green or yellow-green) crystallize in the monoclinic system, C2c group (where x ε (0; 2)). Their structural parameters have the values for Cu2-xMgxP4O12 or Ni2-xMgxP4O12 (X = 2 to x = 0) : a = 11.749(5) to 12.546(7) or 11.644(5) Å, b = 8.278(4) to 8.092(5) or 8.236(4) Å, c = 9.905(4) to 9.565(5) Or 9.813 Å and β = 118.92(2)° to 118.63(3)° or 118.53(2)°, respectively.  相似文献   

18.
The ternary transition metal chalcogenides AxM6X8 (A=Tl, K; M=V, Ti; X=S, Se) build up a three dimensional framework with large hexagonal channels running parallel to the crystallographic c-axis. The electropositive elements thallium or potassium are confined within these channels. It is possible to remove the Tl or K atoms via a chemical redox reaction with an I2/CH3CN solution or with H2O. Using SEM it is demonstrated that the host matrix “V6S8” is only slightly affected by the redox agent. In contrast the host matrix “Ti6Se8” of TlxTi6Se8 reacts with the I2/CH3CN solution. The results of the EDXS analyses clearly show that the removal of the electropositive elements proceeds only along the large channels and not through the host matrix.  相似文献   

19.
About Glass Formation and Properties of Chalcogenide Systems. XXXIII. Condensed Thio- and Selenohypodigermanates and -silicates Na8M4X10 (M?Si, Ge) and Na4Ge4X8 (X?S, Se) The formation of the compounds Na8Si4X10 and Na8Ge4X10 (X?S, Se) is reported prepared by reaction of Ge2S3 or Ge2Se3 with Na2S or Na2Se, respectively, in CH3OH utilizing a mole ratio of 1 to 2 or in the case of the Si compounds by synthesis from the elements. Applying the mole ratio Ge2X3:Na2X = 1 the compounds Na4Ge4X8 (X?S, Se) are obtained. The anion constitution is discussed in relation with cryoscopic mole weight measurements in Glauber-salt melts.  相似文献   

20.
Synthesis, Structure, and Properties of the Tantalum‐rich Silicide Chalcogenides Ta15Si2QxTe10–x (Q = S, Se) The quaternary tantalum silicide chalcogenides Ta15Si2QxTe10–x (Q = S, Se) are accessible from proper, compacted mixtures of the respective dichalcogenides, silicon and elemental tantalum at 1770 K in sealed molybdenum tubes. The structures were determined from the strongest X‐ray intensities of fibrous crystals with cross sections of about 3 μm and confirmed by fitting the profile of single phase X‐ray diffractograms. The phases Ta15Si2S3.5Te6.5 and Ta15Si2Se3.5Te6.5 crystallize in the monoclinic space group C2/m with two formula units per unit cell, a = 2393.7(1) pm, b = 350.08(2) pm, c = 1601.2(1) pm, β = 124.700(4)°, and a = 2461.3(2) pm, b = 351.70(2) pm, c = 1601.7(1) pm, β = 124.363(5)°, respectively. Tri‐capped trigonal prismatic Ta9Si clusters stabilized by encapsulated Si atoms can be seen as the characteristic unit of the structure. The clusters are fused into twin columns which are connected by additional Ta atoms, thus forming corrugated layers. The remaining valences at the surfaces of the layered Ta–Si substructure are saturated by those of chalcogen atoms which are coordinated only from one side by three, four or five Ta atoms. Few bridging covalent Ta–S–Ta and Ta–Se–Ta bonds and, otherwise, dispersive interactions between the Q atoms hold these nearly one nanometer wide slabs together. The phases are moderate metallic conductors. There is no evidence for any electronic instability within 10–310 K in spite of the high anisotropy of the structures.  相似文献   

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