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1.
In this study, nano-scale precursors of ZnO, SiO2, and MnO2 powders were used to prepare mixtures with the compositions of 2ZnO+SiO2+X mol% MnO2 (X=MnO2/2ZnO, abbreviated as Zn2SiO4-X-MnO2), where 2≤X≤5. The mixed Zn2SiO4-X-MnO2 mixtures were calcined from 900 to 1300 °C in air in order to synthesize Zn2SiO4:Mn2+ green phosphors. The X-ray diffraction patterns of Zn2SiO4-X-MnO2 particles indicated that ZnO was present in the 900 °C-calcined Zn2SiO4-X-MnO2 phosphors, but not in particles calcined at temperatures of 1000 °C and higher. However, the unapparent secondary phase of ZnMnO3 was found in the 1200 and 1300 °C-calcined Zn2SiO4-5-MnO2 compositions. The luminescent characteristics of Zn2SiO4-X-Mn2+ phosphors were compared with that of a commercial product (Nichia Corp., Japan). The photoluminescence (PL) intensity of 1200 °C-calcined Zn2SiO4-4-MnO2 phosphors was higher and the decay times of all synthesized Zn2SiO4-X-MnO2 phosphors were longer than those of the commercial product.  相似文献   

2.
TiO2/SiOx double-layers have been prepared at room temperature by RF magnetron sputtering. The TiO2 top-layer was deposited in an Ar atmosphere, while the SiOx bottom-layer was deposited in an Ar/O2 atmosphere. Samples were characterized using X-ray photoelectron spectroscopy, scanning electron microscopy, atomic force microscopy, and photoluminescence techniques. The photocatalytic activity of the samples was evaluated by the photodegradation of methylene blue; the results showed that the photocatalytic activity of the TiO2/SiOx double-layers was superior to that of the TiO2 single-layers. The presence of the SiOx bottom-layer improved the photocatalytic activity of the TiO2 layer because it may act as a trap for electrons generated in the TiO2 layer thus preventing electron-hole recombinations.  相似文献   

3.
The influence of SiO2 on the electrical transport properties of LCMO/SiO2 composites with different SiO2 contents x is investigated, where LCMO represents La2/3Ca1/3MnO3. Results show that the SiO2 phase not only shifts the metal–insulator transition temperature (Tp) to a high temperature range, but also has an effect on the magnetoresistance (MR) of the composites. The temperature dependence of resistivity indicates that the Tp of the composites is obviously higher than that of pure LCMO, and that the peak resistivity ρmax of the composites is lower than that of pure LCMO. In the SiO2 content x∼0.02, the TP is the highest and ρmax becomes the lowest. The experimental observation is discussed on the basis of the analysis of scanning electron microscopy (SEM) images and X-ray diffraction (XRD) patterns. Compared with pure LCMO, a possible interpretation is presented by considering the influence of SiO2 on the coupling between ferromagnetic (FM) domains of LCMO.  相似文献   

4.
Binary Al2O3/SiO2-coated rutile TiO2 composites were prepared by a liquid-phase deposition method starting from Na2SiO3·9H2O and NaAlO2. The chemical structure and morphology of binary Al2O3/SiO2 coating layers were investigated by Fourier transform infrared spectroscopy, X-ray photoelectron spectroscopy, TG-DSC, Zeta potential, powder X-ray diffraction, and transmission electron microscopy techniques. Binary Al2O3/SiO2 coating layers both in amorphous phase were formed at TiO2 surfaces. The silica coating layers were anchored at TiO2 surfaces via Si-O-Ti bonds and the alumina coating layers were probably anchored at the SiO2-coated TiO2 surfaces via Al-O-Si bonds. The formation of continuous and dense binary Al2O3/SiO2 coating layers depended on the pH value of reaction solution and the alumina loading. The binary Al2O3/SiO2-coated TiO2 composites had a high dispersibility in water. The whiteness and brightness of the binary Al2O3/SiO2-coated TiO2 composites were higher than those of the naked rutile TiO2 and the SiO2-coated TiO2 samples. The relative light scattering index was found to depend on the composition of coating layers.  相似文献   

5.
Plasma-enhanced chemical vapor deposition was used to conformally coat commercial TiO2 nanoparticles to create nanocomposite materials. Hexamethyldisiloxane (HMDSO)/O2 plasmas were used to deposit SiO2 or SiOxCyHz films, depending on the oxidant concentration; and hexylamine (HexAm) plasmas were used to deposit amorphous amine-containing polymeric films on the TiO2 nanoparticles. The composite materials were analyzed using Fourier-transform infrared spectroscopy (FTIR), X-ray photoelectron spectroscopy (XPS) and scanning electron microscopy (SEM). These analyses reveal film composition on the nanoparticles was virtually identical to that deposited on flat substrates and that the films deposit a conformal coating on the nanoparticles. The performance of the nanocomposite materials was evaluated using UV-vis spectroscopy to determine the dispersion characteristics of both SiOx and HexAm coated TiO2 materials. Notably, the coated materials stay suspended longer in distilled water than the uncoated materials for all deposited films.  相似文献   

6.
The magnetoresistive effect of CuPt(8 nm)/SiO2(5 nm)/Si(50,000 nm)/SiO2(5 nm)/CuPt(8 nm) structure made by e-beam evaporation technique is studied in this work. Variation in magnetoresistance obtained by I-V measurements at 77 K and in the presence of less than 5 mT magnetic field applied in parallel to the surface is investigated. We have found that this structure exhibit large magnetoresistance in low magnetic fields (i.e. <5 mT). Our results also indicate that the variation in magnetoresistance in the presence of external magnetic field has oscillatory behavior and has the maximum value of 3295%. This structure due to its high sensitivity to low magnetic fields can also be used as an active element in magnetic field sensor devices.  相似文献   

7.
Microstructural properties of liquid and amorphous SiO2 nanoparticles have been investigated via molecular dynamics (MD) simulations with the interatomic potentials that have weak Coulomb interaction and Morse-type short-range interaction under non-periodic boundary conditions. Structural properties of spherical nanoparticles with different sizes of 2, 4 and 6 nm obtained at 3500 K have been studied through partial radial distribution functions (PRDFs), coordination number and bond-angle distributions, and compared with those observed in the bulk. The core and surface structures of liquid SiO2 nanoparticles have been studied in detail. We found significant size effects on structure of nanoparticles. Calculations also show that if the size is larger than 4 nm, liquid SiO2 nanoparticles at the temperature of 3500 K have a lightly distorted tetrahedral network structure with the mean coordination number ZSi-O≈4.0 and ZO-Si≈2.0 like those observed in the bulk. Moreover, temperature dependence of structural defects and SiOx stoichiometry in nanoparticles on cooling from the melt has been found and presented.  相似文献   

8.
SiO2的赝晶化及AlN/SiO2纳米多层膜的超硬效应   总被引:1,自引:0,他引:1       下载免费PDF全文
赵文济  孔明  黄碧龙  李戈扬 《物理学报》2007,56(3):1574-1580
采用反应磁控溅射法制备了一系列不同SiO2层厚度的AlN/SiO2纳米多层膜,利用X射线衍射仪、高分辨透射电子显微镜和微力学探针表征了多层膜的微结构和力学性能,研究了SiO2层在多层膜中的晶化现象及其对多层膜生长方式及力学性能的影响. 结果表明,由于受AlN六方晶体结构的模板作用,溅射条件下以非晶态存在的SiO2层在其厚度小于0.6 nm时被强制晶化为与AlN相同的六方结构赝晶体并与AlN形成共格外延生长. 由于不同模量的两调制层存在晶格错配度,多层膜中产生了拉、压交变的应力场,使得多层膜产生硬度升高的超硬效应. SiO2随层厚的进一步增加又转变为以非晶态生长,多层膜的外延生长结构受到破坏,其硬度也随之降低. 关键词: 2纳米多层膜')" href="#">AlN/SiO2纳米多层膜 赝晶化 应力场 超硬效应  相似文献   

9.
In this work, we report on two properties of the oxidation of tantalum silicide (Ta2Si) on SiC substrates making this material of interest as insulator for many wide bandgap or compound semiconductors. The relatively high oxidation rate of tantalum silicide to form high-k insulator layers and its ability for being oxidized in diluted N2O ambient in a manner similar to the oxidation in O2 are investigated. Metal-insulator-semiconductor capacitors have been used to establish the actual applicability and constrain of the high-k insulator depending on the oxidation conditions. At 1050 °C, the reduction of the oxidation time from 1 h to 5 min affects primordially the SiOx interfacial layer formed between the bulk insulator and the substrate. This interfacial layer strongly influences the metal-insulator-semiconductor performances of the oxidized Ta2Si layer. The bulk insulator basically remains unaffected although some structural differences arise when the oxidation is performed in N2O.  相似文献   

10.
Y.J. Guo  X.T. Zu  B.Y. Wang  X.D. Jiang  X.D. Yuan  H.B. Lv  S.Z. Xu 《Optik》2009,120(18):1012-1015
Two-layer ZrO2/SiO2 and SiO2/ZrO2 films were deposited on K9 glass substrates by sol–gel dip coating method. X-ray photoelectron spectroscopy (XPS) technique was used to investigate the diffusion of ZrO2/SiO2 and SiO2/ZrO2 films. To explain the difference of diffusion between ZrO2/SiO2 and SiO2/ZrO2 films, porous ratio and surface morphology of monolayer SiO2 and ZrO2 films were analyzed by using ellipsometry and atomic force microscopy (AFM). We found that for the ZrO2/SiO2 films there was a diffusion layer with a certain thickness and the atomic concentrations of Si and Zr changed rapidly; for the SiO2/ZrO2 films, the atomic concentrations of Si and Zr changed relatively slowly, and the ZrO2 layer had diffused through the entire SiO2 layer. The difference of diffusion between ZrO2/SiO2 and SiO2/ZrO2 films was influenced by the microstructure of SiO2 and ZrO2.  相似文献   

11.
(Ge:SiO2)/SiO2 multilayers were fabricated for exploring the influence of the stress on the structure of Ge nanocrystals. When annealed at 800 °C, the multilayers show a clear splitting (fine structure) of the Ge (220) X-ray diffraction peak and have a preferred orientation. Similar effects cannot take place in the multilayers annealed at higher or lower temperature. Analyses of Raman scattering, X-ray diffraction spectroscopy, and transmission electron microscope observations suggest that the observed phenomena arise from compressive stress exerted on Ge nanocrystals, which is induced by the confinement of both the SiO2 matrix in the cosputtered layer and neighboring SiO2 layers. The stress may cause an orthorhombic distortion of the diamond structure of bulk Ge. This will lead to the disappearance of the (111) and (311) diffraction peaks and the splitting of the (220) peak. This kind of (Ge:SiO2)/SiO2 multilayers enables us to control the sizes of the Ge crystallites and enhance the stress, and is thus promising in forming new nanocrystal structures.  相似文献   

12.
Thin Cd2Nb2O7 films were grown on single-crystal p-type SiO2/Si substrates by the metallo-organic decomposition (MOD) technique. The films were investigated by X-ray diffraction, X-ray energy-dispersive spectroscopy, and field emission scanning electron microscopy, and showed a single phase (cubic pyrochlore), a crack-free spherical grain structure, and nanoparticles with a mean size of about 68 nm. A Cauchy model was also used in order to obtain the thickness and index of refraction of the stack layers (transparent layer/SiO2/Si) by spectroscopic ellipsometry (SE). The dielectric constant (K) of the films was calculated to be about 25 from the capacitance-voltage (C-V) measurements.  相似文献   

13.
XPS results on two series of catalysts, namely Mo/SiO2 and CoMo/SiO2 in the oxidic form, are reported. In the first series the molybdenum oxide content deposited on SiO2 ranges from 2.8 to 20.6 weight %. The second series was obtained by cobalt impregnation of the first series; in this case the atomic ratio Co/(Co + Mo) was fixed at 0.36.XPS binding energy and intensities measurements enable estimation of the interaction and dispersion between the oxide phase and the support to be made.In the case of molybdenum deposited alone on the support, the binding energies of the Mo and O levels both increase with MoO3 content. When cobalt is also present on the support, the binding energies of the Mo and O levels remain constant. The relative intensities IMo/ISi and ICo/ISi remain constant up to 12% active phase and then drastically increase for higher amounts of oxide.These results confirm the existence of a relatively strong Mo/SiO2 interaction. This interaction is substantially weaker when Co is supported on the MoSiO2 solid, leading to the formation of CoMoO4 at the expense of the Mo/SiO2 interaction. Furthermore, it is shown that at high content of oxide the active phase is deposited on the outer surface of the particle and not inside the pores.  相似文献   

14.
利用射频磁控溅射方法,在n+-Si衬底上淀积SiO2/Si/SiO2纳米双势垒单势阱结构,其中Si层厚度为2至4nm,间隔为0.2nm,邻近n+-S i衬底的SiO2层厚度固定为1.5nm,另一SiO2层厚度固定为3nm.为了 对比研究,还制备了Si层厚度为零的结构,即SiO2(4.5nm)/n+-Si 结构.在经过600℃氮气下退火30min,正面蒸上半透明Au膜,背面也蒸Au作欧姆接触后,所 有样品都在反向偏置(n-Si的电压高于Au电极的电压)下发光,而在正向偏压 下不发光.在一定的反向偏置下,电流和电致发光强度都随Si层厚度的增加而同步振荡,位 相相同.所有样品的电致发光谱都可分解为相对高度不等的中心位于2.26eV(550nm)和1.85eV (670nm)两个高斯型发光峰.分析指出该结构电致发光的机制是:反向偏压下的强电场使Au/( SiO2/Si/SiO2)纳米双势垒/n+-Si结构发生了雪崩击穿 ,产生大量的电子-空穴对,它们在纳米SiO2层中的发光中心(缺陷或杂质)上复 合而发光. 关键词: 电致发光 纳米双势垒 高斯型发光峰 雪崩击穿  相似文献   

15.
The CaCu3Ti4O12/SiO2/CaCu3Ti4O12 (CCTO/SiO2/CCTO) multilayered films were prepared on Pt/Ti/SiO2/Si substrates by pulsed laser deposition method. It has been demonstrated that the dielectric loss and the leakage current density were significantly reduced with the increase of the SiO2 layer thickness, accompanied with a decrease of the dielectric constant. The CCTO film with a 20 nm SiO2 layer showed a dielectric loss of 0.065 at 100 kHz and the leakage current density of 6×10−7 A/cm2 at 100 kV/cm, which were much lower than those of the single layer CCTO films. The improvement of the electric properties is ascribed to two reasons: one is the improved crystallinity; the other is the reduced free carriers in the multilayered films.  相似文献   

16.
A study on interface states density distribution and characteristic parameters of the In/SiO2/p-Si (MIS) capacitor has been made. The thickness of the SiO2 film obtained from the measurement of the corrected capacitance in the strong accumulation region for MIS Schottky diodes was 220 Å. The diode parameters from the forward bias I-V characteristics such as ideality factor, series resistance and barrier heights were found to be 1.75, 106-112 Ω and 0.592 eV, respectively. The energy distribution of the interface state density Dit was determined from the forward bias I-V characteristics by taking into account the bias dependence of the effective barrier height. The interface state density obtained using the I-V characteristics had an exponential growth, with bias towards the top of the valance band, from 9.44×1013 eV−1 cm−2 in 0.329-Ev eV to 1.11×1013 eV−1 cm−2 in 0.527-Ev eV at room temperature. Furthermore, the values of interface state density Dit obtained by the Hill-Coleman method from the C-V characteristics range from 52.9×1013 to 1.11×1013 eV−1 cm−2 at a frequency range of 30kHz-1 MHz. These values of Dit and Rs were responsible for the non-ideal behaviour of I-V and C-V characteristics.  相似文献   

17.
The dielectric properties of MgO-Ta2O5 continuous composition spread (CCS) thin films were investigated. The MgO-Ta2O5 CCS thin films were deposited on Pt/Ti/SiO2/Si substrates by off-Axis RF magnetron sputtering system, and then the films were annealed at 350 °C with rapid thermal annealing system in vacuum. The dielectric constant and loss of MgO-Ta2O5 CCS thin films were plotted via 1500 micron-step measuring. The specific point of Ta2O5-MgO CCS thin film (post annealed at 350 °C) showing superior dielectric properties of high dielectric constant (k ∼ 28) and low dielectric loss (tan δ < 0⋅004) at 1 MHz were found in the area of 3-5 mm apart from Ta2O5 side on the substrate. The cation's composition of thin film was Mg:Ta = 0.4:2 at%.  相似文献   

18.
High-k Ti1−xSixO2 gate dielectric layers were prepared at room temperature by RF magnetron sputtering using SiO2 and TiO2 targets to investigate their applicability to transparent thin-film transistors as well as metal-oxide-semiconductor field-effect transistors. Based on XRD and XPS analyses, it was found that, regardless of the deposition time, the Ti1−xSixO2 gate dielectric layers had more stable Si-based phases with stronger Si-O bonds with increasing SiO2 RF power. As SiO2 RF power increased, the capacitance of the dielectric layers decreased due to the higher fraction of the Si-based phases, and the leakage current decreased, dominantly because of the decrease in oxygen vacancies due to the formation of stoichiometric SiO2. The Ti1−xSixO2 gate dielectric layers exhibited high transparency above 80% and moderate bandgap of 4.1-4.2 eV, which can be applied to transparent thin-film transistors.  相似文献   

19.
Amorphous Lu2O3 high-k gate dielectrics were grown directly on n-type (100) Si substrates by the pulsed laser deposition (PLD) technique. High-resolution transmission electron microscope (HRTEM) observation illustrated that the Lu2O3 film has amorphous structure and the interface with Si substrate is free from amorphous SiO2. An equivalent oxide thickness (EOT) of 1.1 nm with a leakage current density of 2.6×10−5 A/cm2 at 1 V accumulation bias was obtained for 4.5 nm thick Lu2O3 thin film deposited at room temperature followed by post-deposition anneal (PDA) at 600 °C in oxygen ambient. The effects of PDA process and light illumination were studied by capacitance-voltage (C-V) and current density-voltage (J-V) measurements. It was proposed that the net fixed charge density and leakage current density could be altered significantly depending on the post-annealing conditions and the capability of traps to trap and release charges.  相似文献   

20.
A thorough investigation of the catalysts Mo1Te1Ox/SiO2 and Mo1Bi0.05Te1Ox/SiO2 in the partial oxidation of propane is presented in this paper, in order to elucidate the nature and behavior of the active surface. The catalysts’ structures and redox properties were investigated by means of X-ray powder diffraction, Raman spectroscopy, in situ Raman spectroscopy, X-ray photoelectron spectroscopy, and H2-TPR techniques. The results indicate that Te-polymolybdate is the main active phase on fresh catalysts. During reaction, the catalysts underwent a progressive reduction, resulting in the reconstruction of the active surface and the formation of a MoO3 phase. The synergistic effect between Te-polymolybdate and MoO3 was assumed to promote catalytic performance. The different stabilities of Mo1Te1Ox/SiO2 and Mo1Bi0.05Te1Ox/SiO2 catalysts are also discussed.  相似文献   

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