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1.
Etching of amorphous Al2O3 and polycrystalline Y2O3 films has been investigated using an inductively coupled reactive ion etch system. The etch behaviour has been studied by applying various common process gases and combinations of these gases, including CF4/O2, BCl3, BCl3/HBr, Cl2, Cl2/Ar and Ar. The observed etch rates of Al2O3 films were much higher than Y2O3 for all process gases except for Ar, indicating a much stronger chemical etching component for the Al2O3 layers. Based on analysis of the film etch rates and an investigation of the selectivity and patterning feasibility of possible mask materials, optimized optical channel-waveguide structures were fabricated in both materials. In Al2O3, channel waveguides were fabricated with BCl3/HBr plasma and using a standard resist mask, while in Y2O3, channel waveguides were fabricated with Ar and using either a resist or a sputter deposited Al2O3 mask layer. The etched structures in both materials exhibit straight sidewalls with minimal roughness and sufficient etch depths (up to 530 nm for Al2O3 and 250 nm for Y2O3) for defining waveguides with strong optical confinement. Using the developed etch processes, low additional optical propagation losses (on the order of 0.1 dB/cm) were demonstrated in single-mode ridge waveguides in both Al2O3 and Y2O3 layers at 1550 nm. PACS 42.70.-a; 42.82.-m; 42.82.Cr  相似文献   

2.
High resolution photoelectron spectra from transition metal ions in TiO2, V2O5, VO2, V2O3, MnO, Mn2O3, MnO2, Cr2O3, FeO, CoO, NiO, CuO, Cu2O, FeSrO3, and Cu doped CaTiO3 were re-examined using a constrained curve fitting approach. Effective fits of the multiplet splitting present could be attained for the oxides with unfilled 3d bands if multiple final states were assumed. The type of transitions implied, also suggest the classification of these oxides during core level photoelectron emission as either; Mott–Hubbard (V2O5, VO2, V2O3, Cr2O3, and FeO), intermediate (MnO, Mn2O3, and MnO2) or charge transfer type compounds (FeSrO3, CoO, NiO, CuO and Cu doped CaTiO3). These transitions along with relationships defining the splitting energy with respect to the total spin and binding energy are discussed.  相似文献   

3.
The effectiveness of sintering additives for β-SiC was examined based on thermodynamic calculations and experimental observations under hot pressing conditions of 1700–1800 °C. Various types of oxides, such as Al2O3, Fe2O3, MgO, TiO2, WO3 and Y2O3, were examined theoretically by considering the Gibbs formation free energy and vapor pressure. According to experimental observations expanded to their binary and ternary systems after hot pressing at 1750 °C and 20 MPa, Al2O3, MgO, Y2O3 and their mixed systems were found to be the only effective sintering additives that do not react with β-SiC at high temperatures. On the other hand, Fe2O3, TiO2, WO3 and their combinations with other oxides were not effective because of the reaction with β-SiC by forming the corresponding metal carbides and/or silicides, as predicted by thermodynamic simulations. Moreover, the experimental results for the additional possible components were also included.  相似文献   

4.
LiCaBO3:M (M=Eu3+, Sm3+, Tb3+, Ce3+, Dy3+) phosphors were synthesized by a normal solid-state reaction using CaCO3, H3BO3, Li2CO3, Na2CO3, K2CO3, Eu2O3, Sm2O3, Tb4O7, CeO2 and Dy2O3 as starting materials. The emission and excitation spectra were measured by a SHIMADZU RF-540 UV spectrophotometer. And the results show that these phosphors can be excited effectively by near-ultraviolet light-emitting diodes (UVLED), and emit red, green and blue light. Consequently, these phosphors are promising phosphors for white light-emitting diodes (LEDs). Under the condition of doping charge compensation Li+, Na+ and K+, the luminescence intensities of these phosphors were increased.  相似文献   

5.
This paper reports fundamental defect energies in CsF, β-CsCl, CaBr2, CaI2, Ga2O3, Ti2O3, Rh2O3 and V2O3 obtained by simple extrapolation procedures, and in CaCl2 by direct atomistic simulation. It is suggested that CsF, β-CsCl and CaBr2 will exhibit mixed lattice disorder, and that in Ti2O3, Rh2O3 and V2O3 Schottky and anion Frenkel energies differ by less than 1 eV. The implications of mixed disorder for the interpretation of Arrhenius energies of diffusion are examined. For CsF and β-CsCl these are shown to be of the usual type, whereas the temperature dependence of the diffusion coefficients in CaBr2 is predicted to be more complicated.  相似文献   

6.
The inorganic colored composite pigments, such as Fe2O3-, Bi4Ti3O12-, and CoAl2O4-coated mica-titania composites, were prepared by hydrolysis of FeCl3, Bi(NO3)3, and Co(NO3)2/Al(NO3)3 in the presence of mica-titania substrate and calcination at different temperatures. The inorganic coating layers on mica-titania substrate surfaces were explored by X-ray diffraction, scanning electron microscopy, Fourier transform infrared, and X-ray photoelectron spectroscopy. Dense and uniform Fe2O3 coating layers were formed on the surfaces of mica-titania substrates. At lower Bi2O3 loading, Bi4Ti3O12 nanoparticles were formed on the surfaces of mica-titania substrates. But at higher Bi2O3 loading, Bi4Ti3O12 nanosheets were formed and perpendicularly oriented to the substrate surfaces. CoAl2O4 nanosheets were formed on the mica-titania substrates and perpendicularly oriented to the substrate surfaces. The pigmentary performances of the inorganic composite pigments were analyzed by CIE, indicating that red, yellow, and blue colored pigments were achieved by coating Fe2O3, Bi4Ti3O12, and CoAl2O4 on mica-titania substrate surfaces, respectively. The pigmentary performances of the inorganic composite pigments were significantly affected by the morphology and loading of inorganic coating layers.  相似文献   

7.
The effect of additions on the densification of previously prepared stoichiometric barium hexaferrite, during the initial and intermediate stages of sintering, as well as on the coercivity and remanence were studied. The effect of non-stoichiometry, SiO2, Al2O3, Cr2O3, TiO2, SnO2, MnO2, MgO, NiO and Bi2O3 is included.While SiO2 and Bi2O3 form liquid phases that increase the density, Al2O3, Cr2O3 and MnO2 form a limited solid solution and are generally beneficial when added in the proper amounts. At 1300 SiO2 up to 0.55% and Al2O3 up to 1% gave better magnetic properties. On the other hand addition of TiO2, MgO, NiO or SnO2 has a deleterious effect.  相似文献   

8.
The Auger spectra of the iron oxides have been investigated. The relative amplitudes of the Auger lines from oxygen and iron have been determined for FeO, Fe3O4, α-Fe2O3, γ-Fe2O3, and FeOOH. It was found that the amplitude ratio s of the O (510 eV)/Fe (703 eV) lines was, to a first approximation, directly proportional to the ratio of oxygen and iron in the chemical formula. Structure was observed in the spectra resulting from the Fe M2,3 VV transition. Different spectra were observed for Fe, FeO, Fe3O4, Fe3O3, and FeOOH; however, the same spectra were obtained for α- and γ-Fe2O3.  相似文献   

9.
By using very small amount – 11‐mg – of sample powder, major oxides (Na2O, MgO, Al2O3, SiO2, P2O5, K2O, CaO, TiO2, MnO, and total Fe2O3) in ancient pottery (and igneous rocks) were determined with X‐ray fluorescence spectrometry. This minimized amount of sample was used to prepare a fused glass bead with 300 times the weight of lithium tetraborate as an alkali flux. Calibration standards were obtained by compounding chemical reagents (Na2CO3, MgO, Al2O3, SiO2, Na4P2O7, K2CO3, CaCO3, TiO2, MnO2, and Fe2O3) and the flux. Fewer 11 mg of reagents as oxides were able to give reliable calibration curves with good linearity (correlation coefficient: r > 0.995). Fewer 11 mg of sample was able to give reliable analytical results with good precision (relative standard deviation: <3% for more than 10.0 mass% of analyte, <10% for 1.0–10.0 mass% of analyte, and <20% for 0.1–1.0 mass% of analyte). Lower limits of detection were roughly a sub‐percentage of analyte in an unprepared sample (e.g. 0.3 mass% for Na2O, 0.5 mass% for MgO, 1.0 mass% for Al2O3, and 0.01 mass% for MnO). Composition of major oxides in artificial and natural aluminosilicate materials (including rock, stone, sand, sediment, and clay; and their products) should be fundamental information to be considered in detail. The present X‐ray determination based on very small amount of sample might be made readily accessible for destructive analysis of precious samples for archaeology (and geochemistry). Copyright © 2011 John Wiley & Sons, Ltd.  相似文献   

10.
Alumina and 1:1 mixed oxides of Al2O3-ZrO2, Al2O3-TiO2, SiO2-TiO2 and ZrO2-TiO2 were synthesized via a sol-gel process by the so-called neutral amine route, followed by calcination at 600 °C. The mixed oxides were characterized before calcination by X-ray diffraction, revealing ordered hexagonal (Al2O3, Al2O3-ZrO2, ZrO2-TiO2) and lamellar (SiO2-TiO2, Al2O3-TiO2) structures. After calcination, all samples exhibited amorphous structures. Surface areas and pore characteristics of all materials were determined by nitrogen adsorption isotherms. The calcined oxides are active catalysts in the epoxidation of cyclooctene with tert-butyl hydroperoxide as oxidant. Epoxide yields from 14 to 45% were found for reaction times of 24 h. The titanium oxide containing catalysts are the most active and selective ones. On the other hand, the poisoning of acidic centers yields a decreasing activity while increasing selectivity.  相似文献   

11.
《Solid State Ionics》1988,27(4):233-241
H3O+β″Al2O3, H3O+/βAl2O3 and H3O+β″/βAl2O3 /ZrO2 ceramics of equiaxed, fine-grained microstructure were prepared by conventional synthesis techniques, gas-phase and vapour-phase ion exchange to the potassium form and field-assisted ion exchange in dilute HCl vapour to the hydronium form. The bend strength of the polycrystalline H3O+β″Al2O3 and H3O+β″/βAl2O3 was > 200 MPa. The conductivity of H3O+β″Al2O3, H3O+β″/βAl2O3 ZrO2 was 8×10−6, 2×10−6 and 9×10−7 (Ω cm)−1, respectively, at 25°C. The materials were demonstrated to perform in steam electrolysis cells at 100°C.  相似文献   

12.
The time resolved product formation in oxidation of dimethyl ether (DME) has been studied between 298-625 K and 20-90 torr total pressure. Near-infrared frequency modulation spectroscopy (FMS) with Herriott type multi pass optics and UV absorption spectroscopy (UV) were conducted in the same cell. The reaction was initiated by pulsed photolysis in a mixture of Cl2, O2, and DME via CH3OCH2 radical formation. The reaction process was investigated through FMS measurement of HO2 and OH, and UV measurement of CH3OCH2O2. The yields of HO2 and OH are obtained by comparison with reference mixtures, Cl2, O2, and CH3OH for HO2, and Cl2, O2, CH3OH, and NO for OH, which convert 100% of initial Cl to HO2 and OH. The CH3OCH2O2 yield is also obtained. It was found that the HO2 yield increases sharply over 500 K mainly with a longer time constant than that of R + O2 reaction, while a prompt component exists throughout the temperature range at a few percent yield. OH was found to be produced promptly at a yield considerably larger than that known for the simplest alkanes. The CH3OCH2O2 profile has a prompt rise followed by a gradual decay whose rate is consistent with the slow HO2 formation. The species profiles were successfully predicted with a model constructed by modifying the existing one to suit the reduced pressure condition. After modification, it was inferred that the HO2 formation over 500 K is secondary from HCHO + OH and HCO + O2 and a part of HCO is formed directly from the O2 adduct, whereas the HO2 formation below 500 K is governed by CH3OCH2O2 chemistry. The HCO forming pathway via isomerization-decomposition of the O2 adduct, which was not included in the former models, was supported by our quantum-chemical calculations.  相似文献   

13.
Spectra of Eu3+ in various dielectric matrices (Gd2O3:Eu3+, Y2O3:Eu3+, Eu2O3, and mSiO2/Gd2O3:Eu3+ mesoporous particles) are studied by local cathodoluminescence. The results allowed identification of the local environment of Er3+ ions in amorphous samples and detection of the monoclinic Eu2O3 phase impurity in samples with yttrium oxide. The cathodoluminescence spectra of chemically pure Y2O3, Eu2O3, and Gd2O3 are recorded. Conclusions about the structural features of the materials are made and confirmed by other methods (XRD and EPMA).  相似文献   

14.
本文报导了少量稀土元素氧化物(La2O3,CeO2,Sm2O3,Gd2O3和Y2O3)对于一种含ZnO和CuO的Mg-Mn矩磁铁氧体磁心性能的影响,简要地叙述了样品的制备过程。测量了磁心的静态磁滞迴线,饱和磁化强度,居里点和讯号杂音比。实验结果表明:加La2O3或Gd2O3可以增加矩形比和(B-Hm/2)/Bm和讯号杂音比,并使后者的分布往高比值移动,但加CeO2,Sm2O3或Y2O3却没有使这些性能改善,甚至有所降低。文中举例说明了磁心尺寸对于矩形比、淬火温度和稀土元素氧化物的含量对于讯号杂音比的影响。最后指出:这种方法可能提供一种改善磁心某些性能而不显著改变其居里点的途径。  相似文献   

15.
In this study, Sr2P2O7 was doped with some rare earth oxides (Pr6O11, Nd2O3, Dy2O3, Ho2O3, Er2O3, and Tm2O3) at 0.5%, 1%, 2%, 3%, 4%, 5%, 10%, and 15% (by weight) and co-doped with CuO by heating at 900 °C for 10 h. Structural analysis of the products was carried out by powder X-ray diffraction (XRD). XRD patterns of the samples showed that doping did not alter the orthorhombic structure of the Sr2P2O7. Thermoluminescence (TL) glow curve measurements were obtained and these showed that Pr and Cu-doped Sr2P2O7 exhibit very significant thermoluminescence glow peaks, suggesting these could be promising dosimetric materials. Bearing this in mind, some TL dosimetric properties of Sr2P2O7:Cu,Pr compounds are presented in this paper, confirming they are promising for this application.  相似文献   

16.
The electronic structure and optical properties of N-doped β-Ga2O3 and N-Zn co-doped β-Ga2O3 are investigated by the first-principles calculation. In the N-Zn co-doped β-Ga2O3 system, the lattice parameters of a, b, c, V decrease and the formation energy of N-Zn co-doped β-Ga2O3 is smaller in comparison with N-doped β-Ga2O3. There are two shallower acceptor impurity levels in N-Zn co-doped β-Ga2O3. Comparing with N-doped β-Ga2O3, the major absorption peak is red-shifted and the impurity absorption edge is blue-shifted for N-Zn co-doped β-Ga2O3. The results show that the N-Zn co-doped β-Ga2O3 is found to be a better method to push p-type conductivity in β-Ga2O3.  相似文献   

17.
利用热中子透射法测定γ-Fe2O3的氢含量。利用差热分析、磁分析以及穆斯堡尔效应研究γ-Fe2O3的相变,实验结果表明在γ-Fe2O3结构中确实含有一定量的氢,当γ-Fe2O3结构中的阳离子空位被H1+,Co2+,Si4+,P5+等离子占据时,将 关键词:  相似文献   

18.
Samples of the iron oxides Fe0.94O, Fe3O4, Fe2O3, and Fe2SiO4 were prepared by high temperature equilibration in controlled gas atmospheres. The samples were fractured in vacuum and high resolution XPS spectra of the fractured surfaces were measured. The peak positions and peak shape parameters of Fe 3p for Fe2+ and Fe3+ were derived from the Fe 3p XPS spectra of the standard samples of 2FeO·SiO2 and Fe2O3, respectively. Using these parameters, the Fe 3p peaks of Fe3O4 and Fe1−yO are analysed. The results indicate that high resolution XPS techniques can be used to determine the Fe2+/Fe3+ ratios in metal oxides. The technique has the potential for application to other transition metal oxide systems.  相似文献   

19.
The Mössbauer determined cation distributions of FeV2O4, FeCr2O4, FeMn2O4, Fe3O4, FeCo2O4, CoV2O4, CoCr2O4, CoMn2O4, CoFe2O4 and Co3O4 are compared with the quantitative d-orbital stablization energies of McClure and of Dunitz and Orgel. They are also compared with the qualitative ligand field stabilization energies of Cotton. These theories do not account for observation in the cases of FeMn2O4, FeCo2O4 and CoFe2O4.  相似文献   

20.
Cobalt-based alloy coatings with and without nano-Y2O3 particles produced by a 5 kW CO2 laser on Ni-based superalloy were introduced. Solidified microstructure, phase compositions and distribution of nano-particles were investigated by using optical microscope, SEM, TEM and XRD. The results showed that metastable phases, such as γ-Co and Cr23C6 existed in cobalt-based alloy coatings. Another two phases (Y2O3 and ?-Co) were found by adding nano-Y2O3. Without nano-Y2O3, rapid directional solidified microstructure of columnar dendrite appeared. Fine and short dendritic microstructure and columnar to equiaxed transition (CET) occurred by adding nano-Y2O3 particles. With the increase in amount of nano-Y2O3, fully equiaxed crystallization appeared and the formation mechanism was analyzed. The results also showed that the sub-microstructure of the coatings changed from dislocation to stacking fault by adding nano-Y2O3.  相似文献   

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