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1.
The non - centrosymmetric tetragonal inverse spinel structure of LiZnNbO4 has been explored with a view to prepare new colored compounds. The substitution of Co2+, Ni2+, Fe2+, Mn2+, and Cu2+ ions were attempted in the place of Zn2+ ions and Sb5+ ions in place of Nb5+ ions. The studies indicated that 0.75 Zn2+ ions in LiZnNbO4 can be replaced by Co2+ ions and 0.5 Zn2+ ions in LiZnNb0.5Sb0.5O4 compound. The substitution of Co2+ ions gives rise to different shades of blue color in Li(Zn1-xCox)NbO4 compounds and from ink blue to blue-green color in Li(Zn1-xCox)(Nb0.5Sb0.5)O4 compounds. The different colors observed in the present study were explained by the traditional allowed d-d transitions as well as the metal-to-metal charge transfer (MMCT) transitions involving Nb5+ (4d0) ions and partially filled 3d electrons. The SHG studies indicate that the prepared compounds are SHG active. All the compounds exhibit reasonable dielectric behavior with low loss. The XPS studies confirm the oxidation states of the different substituted ions. Raman studies indicate variations in the bands due to the substitutions in the parent LiZnNbO4 phase. Magnetic studies on the Co2+ ions substituted compounds suggest antiferromagnetic behavior.  相似文献   

2.
《化学:亚洲杂志》2017,12(20):2734-2743
We explored garnet‐structured oxide materials containing 3d transition‐metal ions (e.g., Co2+, Ni2+, Cu2+, and Fe3+) for the development of new inorganic colored materials. For this purpose, we synthesized new garnets, Ca3Sb2Ga2ZnO12 ( I ) and Ca3Sb2Fe2ZnO12 ( II ), that were isostructural with Ca3Te2Zn3O12. Substitution of Co2+, Ni2+, and Cu2+ at the tetrahedral Zn2+ sites in I and II gave rise to brilliantly colored materials (different shades of blue, green, turquoise, and red). The materials were characterized by optical absorption spectroscopy and CIE chromaticity diagrams. The Fe3+‐containing oxides showed band‐gap narrowing (owing to strong sp–d exchange interactions between Zn2+ and the transition‐metal ion), and this tuned the color of these materials uniquely. We also characterized the color and optical absorption properties of Ca3Te2Zn3−x Cox O12 (0<x ≤2.0) and Cd3Te2Zn3−x Cox O12 (0<x ≤1.0), which display brilliant blue and green‐blue colors, respectively. The present work brings out the role of the distorted tetrahedral coordination geometry of transition‐metal ions and ligand–metal charge transfer (which is manifested as narrowing of the band gap) in producing brilliantly colored garnet‐based materials.  相似文献   

3.
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   

4.
Mechanical activation (MA) of the LiOH+V2O5 and Li2CO3+V2O5 mixtures followed by brief heating at 673 K was used to prepare dispersed Li1+xV3O8. It was shown that structural transformations during MA are accompanied by reduction processes. EPR spectra of Li1+xV3O8 are attributed to vanadyl VO2+ ions with weak exchange interaction. The interaction of localized electrons (V4+ ions) with electron gas (delocalized electrons), which is exhibited through the dependence of EPR line width of vanadium ions versus measurement temperature (C–S–C relaxation), is revealed. It is shown that C–S–C relaxation is different for intermediate and final products. The properties of mechanochemically prepared Li1+xV3O8 are compared with those of HT-Li1+xV3O8, obtained by conventional solid state reaction. Mechanochemically prepared Li1+xV3O8 is characterized by a similar amount of vanadium ions, producing electron gas, but a higher specific surface area.  相似文献   

5.
The stuffed tridymite structure Ba(Zn/Co)1−xSi1−xM2xO4 (M=Al3+ and Fe3+) is explored for the possible multiferroic behavior and to develop new inorganic colored materials. The compounds were synthesized by employing conventional solid-state chemistry methods in the temperature range 1100–1175 °C for 24 h. The powder X-ray diffraction (PXRD) and Rietveld refinement studies indicate that the compounds stabilize in the P63 space group (no. 173). The refinement results were also rationalized by employing Raman spectroscopic studies. The compounds were found to be second harmonic generation (SHG) active and show weak ferroelectric behavior. The co-substitution of Co2+ and Fe3+ in the structure gives rise to a weak ferromagnetic behavior to the compound, BaCo0.75Si0.75Fe0.5O4, making it a multiferroic material. The optical studies on the prepared compounds exhibited blue color (Co2+ in Td geometry), purple color (Ni2+ in Td geometry), and simultaneous substitution of Co2+ and Fe3+ gives rise to blue-green color owing to metal-to-metal charge transfer (MMCT) effect.  相似文献   

6.
YBaCo4O7 compound is capable to intake and release a large amount of oxygen in the temperature range of 200–400°C. In the present study, the effect of Zn, Ga and Fe substitution for Co on the oxygen adsorption/desorption properties of YBaCo4O7 were investigated by thermogravimetry (TG) method. Due to fixed oxidation state of Zn2+ ions, the substitution of Zn2+ for Co2+ suppresses the oxygen adsorption of YBaCo4−xZnxO7. The substitution of Ga3+ for Co3+ also decreases the oxygen absorption capacity of YBaCo4−xGaxO7. This can be explained by the strong affinity of Ga3+ ions towards the GaO4 tetrahedron. Compared with Zn- and Ga-substituted samples, the drop of oxygen adsorption capacity is smallest for Fe-substituted samples because of the similar changeability of oxidation states of Co and Fe ions.  相似文献   

7.
Understanding the effects of intermolecular interactions on metal‐to‐metal charge transfer (MMCT) is crucial to develop molecular devices by grafting MMCT‐based molecular arrays. Herein, we report a series of solvent‐free {Fe2Co2} compounds sharing the same cationic tetranuclear {[Fe(PzTp)(CN)3]2[Co(dpq)2]2}2+ (PzTp?=tetrakis(pyrazolyl)borate, dpq=dipyrido[3,2‐d:2′,3′‐f]quinoxaline) square units but having anions with different size, including BF4?, PF6?, OTf?, and [Fe(PzTp)(CN)3]?. Intermolecular π???π interactions between dpq ligands, which coordinate to cobalt ions in the {[Fe(PzTp)(CN)3]2[Co(dpq)2]2}2+ units, can be modulated by introducing different counterions, regulating the distortion of the CoN6 octahedron and ligand field around the cobalt ions. This change results in different MMCT behavior. Computational analyzes reveal the substantial role of the intermolecular interactions tuned by the presence of different counteranions on the MMCT behavior.  相似文献   

8.
In this work, the g factors, dd transition band, local distortion, and their concentration dependences for impurity V4+ in 20Li2O–20PbO–45B2O3–(15 − x)P2O5:V2O5 (0 ≤ x ≤ 2.5 mol%) glasses are theoretically investigated by using perturbation formulas of g factors for a tetragonally compressed octahedral 3d1 cluster. In the light of the cubic polynomial concentration functions for cubic field parameter Dq, covalency factor N, and relative tetragonal compression ratio ρ, the calculated concentration dependences of dd transition band and g factors for V4+ show good agreement with the experimental data. With increasing x, N (≈0.7682–0.8165) displays the monotonously increasing trend, whereas ρ (≈6.5–4.2%) and Dq (≈1504.9–1481.1 cm−1) exhibit the decreasing tendencies. The above concentration dependences can be ascribed to the modifications of the V4+–O2− bonding and orbital admixtures around the impurity V4+ due to the effects of V2O5 doping on the stability of the glass network, the strength of local crystal fields, and the electron cloud distribution.  相似文献   

9.
Transition metal complexes of type M(L)2(H2O)x were synthesized, where L is deprotonated Schiff base 2,4‐dihalo‐6‐(substituted thiazol‐2‐ylimino)methylphenol derived from the condensation of aminothiazole or its derivatives with 2‐hydroxy‐3‐halobenzaldehyde and M = Co2+, Ni2+, Cu2+ and Zn2+ (x = 0 for Cu2+ and Zn2+; x = 2 for Co2+ and Ni2+). The synthesized Schiff bases and their metal complexes were thoroughly characterized using infrared, 1H NMR, electronic and electron paramagnetic resonance spectroscopies, elemental analysis, molar conductance and magnetic susceptibility measurements, thermogravimetric analysis and scanning electron microscopy. The results reveal that the bidentate ligands form complexes having octahedral geometry around Co2+ and Ni2+ metal ions while the geometry around Cu2+ and Zn2+ metal ions is four‐coordinated. The geometries of newly synthesized Schiff bases and their metal complexes were fully optimized in Gaussian 09 using 6–31 + g(d,p) basis set. Fluorescence quenching data reveal that Zn(II) and Cu(II) complexes bind more strongly to bovine serum albumin in comparison to Co(II) and Ni(II) complexes. The ligands and their complexes were evaluated for in vitro antibacterial activity against Escherichia coli ATCC 25922 (Gram negative) and Staphylococcus aureus ATCC 29213 (Gram positive) and cytotoxicity against lever hepatocellular cell line HepG2.  相似文献   

10.
基于尖晶石晶体结构信息,本文采用热力学三亚晶格模型,将材料热力学计算和第一性原理计算相结合,研究了ZnxMn1-x Fe2O4和NixMn1-xFe2O4立方相中的Zn2+、Ni2+、Mn2+以及Fe3+在8a和16d亚晶格上的占位有序化行为。结果表明:在锰铁氧体中,室温下Mn2+完全占据在8a亚晶格上,Fe3+完全占据在16d亚晶格上,属于正尖晶石结构;随着热处理温度升高,在1 273 K达到热处理平衡时的占位构型为(Fe0.093+Mn0.912+)[Fe1.913+Mn0.092+]O4,在热处理温度升至1 473 K时,达到热处理平衡时的占位构型为(Fe0.113+ Mn0.892+)[Fe1.893+Mn0.112+]O4,均与实验结果符合较好。在锌铁氧体中,室温下Zn2+完全占据在8a亚晶格上,Fe3+完全占据在16d亚晶格上,属于正尖晶石结构;在热处理温度较高时,Zn2+和Fe3+发生部分置换,符合实验结果。在镍铁氧体中,半数的Fe3+在室温下占据在8a亚晶格上,Ni2+与剩下另一半的Fe3+共同占据在16d亚晶格上,仅在热处理温度较高的时候发生微弱变化,亦与已有的实验结果吻合。在此基础上,本文进一步通过热力学预测建立了立方相尖晶石结构的ZnxMn1-xFe2O4、NixMn1-xFe2O4复合体系中阳离子占位行为与热处理温度对占位的影响。  相似文献   

11.
The quest for new oxides with cations containing active lone‐pair electrons (E) covers a broad field of targeted specificities owing to asymmetric electronic distribution and their particular band structure. Herein, we show that the novel compound BaCoAs2O5, with lone‐pair As3+ ions, is built from rare square‐planar Co2+O4 involved in direct bonding between As3+E and Co2+ dz2 orbitals (Co? As=2.51 Å). By means of DFT and Hückel calculations, we show that this σ‐type overlapping is stabilized by a two‐orbital three‐electron interaction allowed by the high‐spin character of the Co2+ ions. The negligible experimental spin‐orbit coupling is expected from the resulting molecular orbital scheme in O3AsE–CoO4 clusters.  相似文献   

12.
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   

13.
The quest for new oxides with cations containing active lone‐pair electrons (E) covers a broad field of targeted specificities owing to asymmetric electronic distribution and their particular band structure. Herein, we show that the novel compound BaCoAs2O5, with lone‐pair As3+ ions, is built from rare square‐planar Co2+O4 involved in direct bonding between As3+E and Co2+ dz2 orbitals (Co As=2.51 Å). By means of DFT and Hückel calculations, we show that this σ‐type overlapping is stabilized by a two‐orbital three‐electron interaction allowed by the high‐spin character of the Co2+ ions. The negligible experimental spin‐orbit coupling is expected from the resulting molecular orbital scheme in O3AsE–CoO4 clusters.  相似文献   

14.
EPR spectroscopy is used to study the electronic state of vanadium ions in HT- and LT-Li1+xV3O8. It is shown that in both cases the EPR spectra observed are attributed to vanadyl VO2+ ions (localized electron centers) with weak exchange interaction. The other type of registered electrons is characterized by larger mobility through a few V5+ ions, i.e., by a higher degree of delocalization (electron gas). Based on the analysis of the temperature dependence of the EPR line width, it is stated that the exchange interaction between localized electron centers proceeds through electron gas (C-S-C relaxation). It is found that HT-Li1+xV3O8 differs from LT-Li1+xV3O8 by the sloping form of its spectrum at g range connected with two types of VO2+ ions different in the direction of the crystal field axis corresponding to a short V=O2+ bond.  相似文献   

15.
Crystal structures and magnetic properties of metal telluromolybdates Co1−xZnxTeMoO6 (x=0.0, 0.1,…,0.9) are reported. All the compounds have an orthorhombic structure with space group P21212 and a charge configuration of M2+Te4+Mo6+O6. In this structure, M ions form a pseudo-two-dimensional lattice in the ab plane. Their magnetic susceptibility measurements have been performed in the temperature range between 1.8 and 300 K. The end member CoTeMoO6 shows a magnetic transition at 24.4 K. The transition temperature for solid solutions rapidly decreases with increasing x and this transition disappears between x=0.4 and 0.5, which is corresponding to the percolation limit for the square-planer lattice. From the magnetization, specific heat, and powder neutron diffraction measurements, it is found that the magnetic transition observed in the CoTeMoO6 is a canted antiferromagnetic ordering of Co2+ ions. The antiferromagnetic component of the ordered magnetic moment (3.12(3)μB at 10 K) is along the b-axis. In addition, there exists a small ferromagnetic component (0.28(3)μB) along the a-axis.  相似文献   

16.
Using the Pechini method, pigments with spinel structure (Zn7Sb2O12)were synthesized by substitution of the cation Zn2+ by Co2+, in compounds with different concentrations of Sb2O3. The doping resulted in CoxZn(7–x)Sb2O12 phases(x=1–7) that were isomorphs to spinel, denominated as samples A and B. After thermal treatment at 400°C for 1 h, the powders were characterized by thermogravimetry(TG) and differential thermal analysis (DTA). The results indicate a different behavior whena higher amount of Sb2O3 is used, due to the presence of a secondary phase (ilmenite). This revised version was published online in July 2006 with corrections to the Cover Date.  相似文献   

17.
The phase and chemical compositions of precipitates formed in the system Zn(VO3)2–HCl–VOCl2–H2O at pH 1?3, molar ratio V4+: V5+ = 0.1?9, and 80°C were studied. It was shown that, within the range 0.4 ≤ V4+: V5+ ≤ 9, zinc vanadate with vanadium in a mixed oxidation state forms with the general formula ZnxV4+ yV5+ 2-yO5 ? nH2O (0.005 ≤ x ≤ 0.1, 0.05 ≤ y ≤ 0.3, n = 0.5?1.2). Vanadate ZnxV2O5 ? nH2O with the maximum tetravalent vanadium content (y = 0.30) was produced within the ratio range V4+: V5+ = 1.5?9.0. Investigation of the kinetics of the formation of ZnxV2O5 ? nH2O at pH 3 determined that tetravalent vanadium ions VO2+ activate the formation of zinc vanadate, and its precipitation is described by a second-order reaction. It was demonstrated that, under hydrothermal conditions at pH 3 and 180°C, zinc decavanadate in the presence of VOCl2 can be used as a precursor for producing V3O7 ? H2O nanorods 50–100 nm in diameter.  相似文献   

18.
A series of 2D isomorphous MOFs [M (HBTC)(BMIOPE)·DMF·H2O]n (M = Zn ( 1 ), Zn0.7Co0.3 ( 2 ), Zn0.5Co0.5 ( 3 ), Zn0.3Co0.7 ( 4 ), Co ( 5 ), H3BTC = 1,3,5-benzenetricarboxylic acid, BMIOPE = 4,4′-bis(2-methylimidazol-1-yl)diphenyl ether) were synthesized to investigate the correction between the center metal ions and the photocatalytic behaviors. The photocatalytic results show that with the increase of Co2+ content, the photodegradation properties are continuously improved from 1 to 5 , which fully indicate that only changing metal ions could regulate the photodegradation properties. In detail, 1 is an inactive photocatalyst to degrade methylene blue (MB), while 5 exhibits preeminent photocatalytic properties under visible light irradiation. Moreover, 1 shows good selective sensing toward Fe3+, Cr3+, UO22+, CrO42− and Cr2O72− ions in aqueous solution. To the best of our knowledge, 1 is the first MOF example for the optical detection of Fe3+, Cr3+, UO22+, CrO42− and Cr2O72− ions in aqueous solution.  相似文献   

19.
Mössbauer spectra of the Fe1+xV2−xO4 spinel solid solutions are taken to investigate the cation distribution. Room temperature spectra can be interpreted by assuming that the cation distribution is represented approximately as Fe2+[Fe3+xV3+2−x]O4 for 0 x 0.35 and Fe3+[Fe2+Fe3+x−1V3+2−x]O4 for 1 x 2 and the ionic valence arrangement changes from the 2-3-3 type (Fe2+[Fe3+xV3+2−x]O4) to the 3-2-3 one (Fe3+[Fe2+V3+]O4) in the range 0.35 x 1. Fe2VO4 is found to be 3-2-3 spinel, Fe3+[Fe2+V3+]O4. Its paramagnetic spectrum at 473°K is, however, composed of a broad single line with isomer shift value of 0.61 mm/sec relative to stainless steel, in which the line splitting due to the ferric and ferrous ions is rendered indistinguishable.  相似文献   

20.
采用高温固相法在空气中合成了Ba1.97-yZn1-xMgxSi2O7:0.03Eu,yCe3+系列荧光粉。分别采用X-射线衍射和荧光光谱对所合成荧光粉的物相和发光性质进行了表征。在紫外光330~360 nm激发下,固溶体荧光粉Ba1.97-yZn1-xMgxSi2O7:0.03Eu的发射光谱在350~725 nm范围内呈现多谱峰发射,360和500 nm处有强的宽带发射属于Eu2+离子的4f65d1-4f7跃迁,590~725 nm红光区窄带谱源于Eu3+5D0-7FJ (J=1,2,3,4)跃迁,这表明,在空气气氛中,部分Eu3+在Ba1.97-yZn1-xMgxSi2O7基质中被还原成了Eu2+;当x=0.1时,荧光粉Ba1.97Zn0.9Mg0.1Si2O7:0.03Eu的绿色发光最强,表明Eu3+被还原成Eu2+离子的程度最大。当共掺入Ce3+离子后,形成Ba1.97-yZn0.9Mg0.1Si2O7:0.03Eu,yCe3+荧光粉体系,其发光随着Ce3+离子浓度的增大由蓝绿区经白光区到达橙红区;发现名义组成为Ba1.96Zn0.9Mg0.1Si2O7:0.01Ce3+,0.03Eu的荧光粉的色坐标为(0.323,0.311),接近理想白光,是一种有潜在应用价值的白光荧光粉。讨论了稀土离子在Ba2Zn0.9Mg0.1Si2O7基质中的能量传递与发光机理。  相似文献   

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