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1.
New lanthanum aluminates LaMAl11O19 (M2+ = Ni, Co, Mn, Mg1?xMnx, 0 ≤ x ≤ 1), with magnetoplumbite-like structure have been obtained as single crystals. This paper is particularly devoted to the Mn2+ and Mg2+Mn2+ mixed compounds, which exhibit promising luminescent properties. Several characteristics of the crystals are given. The absorption spectra of the materials, as grown, are assigned to Mn2+ ions in tetrahedral sites. After annealing in air new absorptions attributed to octahedral Mn3+ ions, appear. The ESR spectra of Mn2+ in all these crystals exhibit axial symmetry. For x ≤ 0.25 they arise from isolated Mn2+ ions in slightly distorted tetrahedral sites and reveal a strong disorder effect. For x ≥0.5 the spectra consist of a single line, attributed to clusters of magnetically interacting Mn2+ ions.  相似文献   

2.
The “114” YBaCo4O7 cobaltite undergoes structural transition just beyond room temperature at TS∼310 K. Correspondingly, its signature in the physical properties is detected by T-dependent measurements of electrical resistivity, magnetic susceptibility and thermoelectric power. It is found that low-level substitutions of divalent (M=Zn2+) or trivalent (M=Ga3+, Al3+) cations for cobalt according to the YBaCo4−xMxO7 formula with x?0.4 have a strong impact upon this transition. On the one hand, Zn2+ substitutions preserve the transition but with TS decreasing as x increases. On the other hand, for x=0.2 Ga3+ or Al3+, the transition is suppressed, i.e., for only 5% trivalent foreign cation substituted for cobalt. Though at first, this contrasted behaviour between divalent and trivalent substituting cations appears to be linked to the opposite evolution of hole carriers “Co3+” concentration with x, a possible destabilization of 3Co2+: 1Co3+ charge ordering induced by the M3+ cations is considered.  相似文献   

3.
The cation ordering in the fluorite-like transparent conductors In4+xSn3−2xSbxO12 and In6TeO12, was investigated by Time of Flight Neutron Powder Diffraction and X-ray Powder Diffraction (tellurate). The structural results including atomic positions, cation distributions, metal-oxygen distances and metal-oxygen-metal angles point to a progressive cation ordering on both sites of the Tb7O12-type structure with a strong preference of the smaller 4d10 cations (Sn4+, Sb5+, Te6+) for the octahedral sites. The corresponding increase of the overall structure-bonding anisotropy is analyzed in terms of the crystal chemical properties of the OM4 tetrahedral network of the antistructure. The relationships between the M7O12 and the M2O3 bixbyite-type structures are explored. Within the whole series of compositions In4+xM3−xO12 (M=Sn, Sb, Te) there exists an increase of the symmetry gap between the more symmetrical bixbyite structure and the M7O12 type. This is tentatively correlated with the progressive weakening of thermal stability of these compositions from Sn to Te via Sb.  相似文献   

4.
Additional Magnetic Examinations of Ti3?xMxO5-Phases (M = Al3+, Fe2+, Mn2+, Mg2+) with a Contribution about CrTi2O5 Ti3?xMxO5 was prepared with M = Al3+, Fe2+, Mn2+, and Mg2+. Die magnetic properties of this phases were examinated by the Faraday method in respect to the temperature. The well known magnetic effect of Ti3O5 near 450 K is shifted to lower degrees if Ti is replaced by Al, Fe, Mn, or Mg. Compared to Ti3?xVxO5 and Ti3?xCrxO5 the stability of the low temperature-form of Ti3O5 is much more reduced in Ti3?xMxO5 (M = Al, Fe, Mn, Mg). The crystal structure investigation of CrTi2O5 explained the anomalous behaviour of the Cr3+ and V3+ doped Ti3O5.  相似文献   

5.
The activity of NiAl2O4 in NiAl2O4MgAl2O4 solid solutions has been measured by using a solid oxide galvanic cell of the type, Pt, Ni + NiAl2O4 + Al2O3(α)/CaOZrO2/Ni + NixMg1?xAl2O4 + Al2O3(α). Pt, in the temperature range 750–1150°C. The activities in the spinel solid solutions show negative deviations from Raoult's law. The cation distribution in the solid solutions has been calculated using site preference energies independent of composition for Ni2+, Mg2+, and Al3+ ions obtained from crystal field theory and measured cation disorder in pure NiAl2O4 and MgAl2O4, and assumi g ideal mixing of cations on the tetrahedral and octahedral positions. The calculated values correctly predict the decrease in the fraction, α, of Ni2+ ions on tetrahedral sites for 1>x>0.25, observed by Porta et al. [J. Solid State Chem.11, 135 (1974)] but do not support their tentative evidence for an increase in α for x < 0.25. The measured excess free energy of mixing can be completely accounted for by using either the calculated or the measured cation distributions. This suggests that the Madelung energy is approximately a linear function of composition in the solid solutions. The composition of NiOMgO solid solutions in equilibrium with NiAl2O4MgAl2O4 solid solutions has been calculated from the results and information available in literature.  相似文献   

6.
Structural and photoluminescence properties of undoped and Ce3+-doped novel silicon-oxynitride phosphors of Ba4−zMzSi8O20−3xN2x (M=Mg, Sr, Ca) are reported. Single-phase solid solutions of Ba4−zMzSi8O20−3xN2x oxynitride were synthesized by partial substitutions of 3O2−→2N3− and Ba→M (M=Mg, Ca, Sr) in orthorhombic Ba2Si4O10. The influences of the type of alkaline earth ions of M, the Ce3+ concentration on the photoluminescence properties and thermal quenching behaviors of Ba3MSi8O20−3xN2x (M=Mg, Ca, Sr, x=0.5) were investigated. Under excitation at about 330 nm, Ba3MSi8O20−3xN2x:Ce3+ (x=0.5) exhibits efficient blue emission centered at 400-450 nm in the range of 350-650 nm owing to the 5d→4f transition of Ce3+. The emission band of Ce3+ shifts to long wavelength by increasing the ionic size of M due to the modification of the crystal field, as well as the Ce3+ concentrations due to the Stokes shift and energy transfer or reabsorption of Ce3+ ions. Among the silicon-oxynitride phosphors of Ba3MSi8O18.5N:Ce3+, M=Sr0.6Ca0.4 possesses the best thermal stability probably related to its high onset of the absorption edge of Ce3+.  相似文献   

7.
The crystal structure of the promising optical materials Ln2M2+Ge4O12, where Ln=rare-earth element or Y; M=Ca, Mn, Zn and their solid solutions has been studied in detail. The tendency of rare-earth elements to occupy six- or eight-coordinated sites upon iso- and heterovalent substitution has been studied for the Y2−xErxCaGe4O12 (x=0-2), Y2−2xCexCa1+xGe4O12 (x=0-1), Y2Ca1−xMnxGe4O12 (x=0-1) and Y2−xPrxMnGe4O12 (x=0-0.5) solid solutions. A complex heterovalent state of Eu and Mn in Eu2MnGe4O12 has been found.  相似文献   

8.
The series of isotypic anhydrous ortho-pyrophosphates MIII(WVIO2)2(P2O7)(PO4) (M: Sc, V, Cr, Fe, Mo, Ru, Rh, In, Ir) was obtained via vapor phase moderated solid state reactions in sealed ampoules. The crystal structure of the phosphates MIII(WVIO2)2(P2O7)(PO4) (M: V, Ru, Rh) was solved from single crystal X-ray data (C2/c, Z = 16). Fairly regular MO6 and distorted WO6 octahedra share vertices with PO4 and P2O7 units to form a 3D network. For the ortho-pyrophosphates with M: V3+, Cr3+, and Fe3+ the oxidation state of M is confirmed by magnetic measurements. 31P-MAS-NMR spectra of the diamagnetic phosphates MIII(WVIO2)2(P2O7)(PO4) (M: Sc, In, Ir) show surprisingly different isotropic chemical shifts for the seven phosphorus sites. VIII(WVIO2)2(P2O7)(PO4) occurs as equilibrium phase in the quasi-binary system (V1–xWx)OPO4 at x = 0.67 and exhibits a small homogeneity range 0.60 ≤ x ≤ 0.67. The scandium compound shows a fully inverted occupancy of the M sites according to the formulation W(Sc1/2W1/2O2)2(P2O7)(PO4).  相似文献   

9.
Series of compositions Bi2(M′xM1−x)4O9 with x=0.0, 0.1,…, 1.0 and M′/M=Ga/Al, Fe/Al and Fe/Ga were synthesized by dissolving appropriate amounts of corresponding metal nitrate hydrates in glycerine, followed by gelation, calcination and final heating at 800 °C for 24 h. The new compositions with M′/M=Ga/Al form solid-solution series, which are isotypes to the two other series M′/M=Fe/Al and Fe/Ga. The XRD data analysis yielded in all cases a linear dependence of the lattice parameters related on x. Rietveld structure refinements of the XRD patterns of the new compounds, Bi2(GaxAl1−x)4O9 reveal a preferential occupation of Ga in tetrahedral site (4 h). The IR absorption spectra measured between 50 and 4000 cm−1 of all systems show systematic shifts in peak positions related to the degree of substitution. Samples treated in 18O2 atmosphere (16 h at 800 °C, 200 mbar, 95% 18O2) for 18O/16O isotope exchange experiments show a well-separated IR absorption peak related to the M-18Oc-M vibration, where Oc denotes the common oxygen of two tetrahedral type MO4 units. The intensity ratio of M-18Oc/M-16Oc IR absorption peaks and the average crystal sizes were used to estimate the tracer diffusion coefficients of polycrystalline Bi2Al4O9 (D=2×10−22 m2s−1), Bi2Fe4O9 (D=5×10−21 m2s−1), Bi2(Ga/Al)4O9 (D=2×10−21 m2s−1) and Bi2Ga4O9 (D=2×10−20 m2s−1).  相似文献   

10.
We report the synthesis of Aurivillius-type phases incorporating magnetic M4+ cations (M=Mn, Ru, Ir), based on the substitution of M4+ for Ti4+ in Bi2Sr2(Nb,Ta)2TiO12. The key to incorporating these magnetic transition metal cations appears to be the partial substitution of Sr2+ for Bi3+ in the α-PbO-type layer of the Aurivillius phase, leading to a concomitant decrease in the M4+ content; i.e., the composition of the prepared compounds was Bi2−xSr2+x(Nb,Ta)2+xM1−xO12, x≈0.5. These compounds only exist over a narrow range of x, between an apparent minimum (x≈0.4) Sr2+ content in the α-PbO-type [Bi2O2] layer required for Aurivillius phases to form with magnetic M4+ cations, and an apparent maximum (x≈0.6) Sr2+ substitution in this [Bi2O2] layer. Rietveld-refinement of synchrotron X-ray powder diffraction data making use of anomalous dispersion at the Nb and Ru K edges show that the overwhelming majority of the incorporated M cations occupy the central of the three MO6 octahedral layers in the perovskite-type block. Magnetic susceptibility measurements are presented and discussed in the context of the potential for multiferroic (magnetoelectric) properties in these materials.  相似文献   

11.
In general, the reduction of Eu3+ to Eu2+ in solids needs an annealing process in a reducing atmosphere. In this paper, it is of great interest and importance to find that the reduction of Eu3+ to Eu2+ can be realized in a series of alkaline-earth metal aluminum silicates MAl2Si2O8 (M=Ca, Sr, Ba) just in air condition. The Eu2+-doped MAl2Si2O8 (M=Ca, Sr, Ba) powder samples were prepared in air atmosphere by Pechini-type sol-gel process. It was found that the strong band emissions of 4f65d1-4f7 from Eu2+ were observed at 417, 404 and 373 nm in air-annealed CaAl2Si2O8, SrAl2Si2O8 and BaAl2Si2O8, respectively, under ultraviolet excitation although the Eu3+ precursors were employed. In addition, under low-voltage electron beam excitation, Eu2+-doped MAl2Si2O8 also shows strong blue or ultraviolet emission corresponding to 4f65d1-4f7 transition. The reduction mechanism from Eu3+ to Eu2+ in these compounds has been discussed in detail.  相似文献   

12.
The AxA2?xLi0.5M0.5O4 matrix deriving from the K2NiF4 structure has an elongated MO6 octahedron; it has been used to stabilize anisotropic electronic configurations such as high-spin Fe4+, low-spin Co4+, medium-spin Co3+, low-spin Ni3+, or low-spin Cu3+. The choice of ions to be stabilized was based on a simple model for predicting the electronic configuration of a dn ion in a tetragonally distorted octahedral environment.  相似文献   

13.
The new compounds Ce2/3−xRh2O4 (x∼0.11-0.14) and CeRh2O5 have been prepared. Their structures were determined from single crystal X-ray diffraction data. Electrical and magnetic properties were also evaluated. Based on the structural analysis and physical properties, oxidation states for CeRh2O5 can be assigned as Ce4+Rh3+2O5. A small variation in x was detected for Ce2/3−xRh2O4 indicating a formula ranging from Ce3.64+0.55Rh3+2O4 to Ce3.81+0.525Rh3+2O4.  相似文献   

14.
CuAl2O4, NiAl2O4, and three ternary spinels CuxNi1?xAl2O3 have been prepared, in polycrystalline form, by solid-state reaction of mixtures of CuO, NiO, and Al2O3 at 1223 K. X-Ray powder diffractometry, coupled with adequate computational methods, allowed determination of the unit-cell length, oxygen positional parameter, and cation distribution for each compound. Interdependence of these structural parameters is closely analyzed on the ternary oxide spinels. The one-electron difference between the Cu2+ and Ni2+ ions was found to be enough to render them distinguishable by X-ray powder diffraction.  相似文献   

15.
The oxyfluoride garnets of formula Y3Fe5?xMxO12?xFx and Gd3Fe5?xMxO12?xFx (M = 3d transition element) result from partial substitution of O2? by F? in Y3Fe5O12 and Gd3Fe5O12 oxides. The cationic charge compensation is obtained by replacing the Fe3+ ions by divalent ions as Mn2+, Co2+, Ni2+, Cu2+ or Zn2+ ions. The site occupied by some of these ions (Mn2+, Ni2+, Zn2+) is determined by magnetic or Mössbauer measurements.  相似文献   

16.
Substitution of Li+ into Co3O4 and ZnCo2O4 gives rise to the solid solution series LixM1?xCo2O4 (M = Co2+ or Zn2+) having the spinel structure upto x = 0.4. X-Ray diffraction intensities show that the spinel solid solutions are likely to have the following cation distributions: (Co2+)t[Li+xCo3+2?3xCo4+2x]0O4 and (Zn2+1?xCo2+x)t[Li+xCo3+2?3xCo4+2x]0O4. Electrical resistivity and Seebeck coefficient data indicate that the electron transport in these systems occurs by a small-polaron hopping mechanism.  相似文献   

17.
Emission properties of Eu2+-doped M3MgSi2O8 (M: Ba, Sr, Ca) are discussed in terms of the crystal structure. When Ba2+ ions account for over one third of M2+ ions, M3MgSi2O8 crystallizes in glaserite-type trigonal structure, while Ba-free compounds crystallize in merwinite-type monoclinic structure. Under UV excitation, the Eu2+-doped glaserite-type compounds exhibit an intense blue emission assigned to 5d-4f electron transition at about 435 nm, regardless of the molar ratio of Ba2+, Sr2+ and Ca2+ ions. By contrast, the Eu2+-doped merwinite-type compounds show an emission color sensitive to the ratio. A detailed analysis of the emission spectra reveals that the emission chromaticity for the Eu2+-doped M3MgSi2O8 is composed of two emission peaks reflecting two different sites accommodating M2+ ion.  相似文献   

18.
Tunneling spectra of Al2O3/—SiHx, MgO/—SiHx, Al2O3/—SiDx, and Al2O3/—SiHx + NCS? are reported. Analysis of the vibrational spectra observed from isotopic substitution of the barriers obtained by deposition of a thin film of SiO onto alumina and magnesia indicate that the supported species is —SiH. The Al2O3/—SiH barrier can be used as a support for studying inorganic ions by IETS.  相似文献   

19.
Cation distribution in quenched and furnace-cooled samples of composition NixM1?xFe2O4 (where M is either Mg2+ or Cu2+) has been studied through magnetization measurements. It has been found that cation distribution in these mixed ferrites cannot be predicted by site preference energies. In magnesium-nickel ferrites, cation distribution is controlled by heat treatment up to x = 0.5, beyond which the effect of heat treatment diminishes. Addition of Ni2+ ions in copper ferrite reduces the diffusibility of Cu2+ ions and the distribution tends toward inverse spinel in the high-nickel region.  相似文献   

20.
Subsolidus phase relations in the CuOx-TiO2-Nb2O5 system were determined at 935 °C. The phase diagram contains one new phase, Cu3.21Ti1.16Nb2.63O12 (CTNO) and one rutile-structured solid solution series, Ti1−3xCuxNb2xO2: 0<x<0.2335 (35). The crystal structure of CTNO is similar to that of CaCu3Ti4O12 (CCTO) with square planar Cu2+ but with A site vacancies and a disordered mixture of Cu+, Ti4+ and Nb5+ on the octahedral sites. It is a modest semiconductor with relative permittivity ∼63 and displays non-Arrhenius conductivity behavior that is essentially temperature-independent at the lowest temperatures.  相似文献   

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