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1.
Qi  Jianquan  Yu  Tianchi  Li  Mengying  Xie  Jiahui  Bo  Cunle  Zhu  Hang  Liu  He  Wang  Hengchang  Xie  Yuxi  Liu  Yilin  Han  Xiumei 《Journal of Materials Science: Materials in Electronics》2021,32(16):21326-21336

In this study, the powders of the Ba0.75Sr0.25TiO3 (BST) nanoparticles were directly synthesized by milling of Ba(OH)2·8H2O, Sr(OH)2·8H2O, and Ti(BuO)4 in ethanol at room temperature. They have homogenous grains of?~?15 nm and high sintering activity. The dense ceramics with the density?>?90% can be obtained at a sintering temperature of?≤?950 °C by adding 3 wt% sintering aids of Bi2O3 and Li2CO3. Several Bi-related intermediate compounds act as perovskite-structured templates to sintering the ceramics at a different temperature. They enhance the mass transfer and promote the sintering densification. These compounds such as Ba2BiO4 and SrBiO4 appear at 800 °C, LiBa4Bi3O11 and Sr1.2Bi0.8O3 appear over 830 °C, and Bi8.11Ba0.89O13.05 appears at 950 °C. The cation Bi in them can have mixture valences of 3+ and 5+. It makes the ceramics as semiconducting state with the dark gray color and decreases the ceramic resistivities. With the sintering temperature increase, especially at 950 °C, the cation Bi tends back to single valence of +3 in the ceramics. The most of alkaline earth cations in Bi-related compounds will release and resorb into the lattice of BST and drive the sintering densification. The BST ceramics can have a peak dielectric constant?>?6500 (at 53 °C) with loss?<?0.025 at 10 kHz, and resistivity?>?1012 Ω cm when sintered at a temperature of?≥?900 °C with 3 wt% sintering aids. They have a potential application for multiple layer ceramic capacitors (MLCC) with silver inner electrodes.

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2.
In order to compare the electrochemical performance of Ce0.9Gd0.1O2−δ (CGO) in various fuels, impedance spectroscopy measurements were carried out in the atmospheres containing H2, CO, CO2, CH4, N2 at various compositions, in the temperature range 650°C to 850°C. Ohmic loss and polarization resistance were derived from impedance spectroscopy measurements. The stability at different temperatures of the anode was also investigated in 9%H2/91%N2 humidified with 3% H2O. The microstructure of the anode before and after degradation test was analysed by SEM. These investigations indicated similarities in the impedance and the activation enthalpies in hydrogen/water, methane/water and CO/CO2 atmospheres. No indications of methane cracking leading to carbon formation were found.  相似文献   

3.
In this work, pure-CaCu3Ti4O12 was successfully prepared by a simple thermal decomposition method. This can easily be achieved by direct firing of starting raw materials dissolved in an aqueous citric acid solution at 800 °C for 6 h. The results show that sintering conditions have a remarkable influence on the microstructure of the CaCu3Ti4O12 ceramics. Interestingly, dense CaCu3Ti4O12 ceramic sintered at 1,050 °C for 2 h exhibits a high dielectric constant of ~5.1 × 103 with low loss tangent of ~0.048 at 30 °C and 1 kHz. The dielectric properties, electrical response of grain boundaries, and related nonlinear current–voltage behavior are found to be associated with the microstructure of CaCu3Ti4O12 ceramics.  相似文献   

4.
Suppressing the crystallization and plate-like crystallite growth of RE2(OH)4SO4·2H2O compound by low-temperature (~4 °C) precipitation produced an amorphous RE2(OH)3.3(CO3)0.35SO4·2H2O precursor (RE = Gd1-xTbx) that can be decomposed to Gd2O2SO4:Tb and Gd2O2S:Tb green phosphor nanopowders of unimodal size distributions upon calcination in air at 1000 °C (average particle size ~156.9 nm) and in hydrogen at 800 °C (average particle size ~130.2 nm), respectively. The optimal RE3+ concentration for precursor synthesis was determined to be ~0.10 mol/L. Through detailed characterization by XRD, FTIR, DTA/TG, FE-SEM, TEM and particle sizing, the courses of phase/morphology evolution were clarified. Photoluminescence study found that the (Gd0.99Tb0.01)2O2SO4 and (Gd0.98Tb0.02)2O2S representative phosphors have quantum efficiencies of ~16.8% (λex = 275 nm) and 38.5% (λex = 286 nm), fluorescence lifetimes of ~3.70 and 1.75 ms and activation energies for thermal quenching of ~0.552 and 0.385 eV, respectively. The values are remarkably larger than those reported for Gd2O2S:Tb, which are considered to be due to higher purity, better crystallization and fewer luminescence-quenching defects of the product. Particularly, the (Gd0.99Tb0.01)2O2SO4 phosphor has negative thermal quenching up to ~150 °C and can retain over 85% of its room temperature emission intensity at 250 °C, which may enlighten its application in high-power LEDs.  相似文献   

5.
X-ray diffraction (XRD) and the X-ray photoelectron spectroscopy (XPS) were measured for the sintered BSCF ceramics (Ba0.5Sr0.5Co x Fe1−x O3−δ, x = 0.2 and 0.8: BSCF5528 and BSCF5582, respectively), which were annealed at different temperatures (700 and 950 °C) and gases (O2 and Ar). The unit cell of the annealed BSCF5528 at 950 °C under Ar expanded by 0.8%, while contracting by 0.45% under O2. The cubic and rhombohedral phases coexist in the BSCF5582 annealed at 700 °C under O2. The XPS peak areas of lattice oxygen (O2−) in O1s , ~528 eV, and the shoulder peak of Co2p /Ba3d in BSCF5582 (~778 eV) increased significantly after being annealed in O2. The areas of the peaks for BaCO3 (87.9/90.2 eV) in Ba4d preferentially were shown to decrease in Ar and increase in O2.  相似文献   

6.
《Optical Materials》2005,27(2):279-283
The chiral organic molecules glucose (C6H12O6) and griseofulvin (C17H17ClO6) were first uniformly incorporated in sol–gel derived materials. The polarity response, absorption spectra and thermal stability were measured and discussed. The DTA results indicated that the C6H12O6 and C17H17ClO6 in gels were stable in air at the temperature lower than 210 and 350 °C, respectively. An absorption band at about 1.4 μm due to OH existed in the infrared absorption spectra of the gels. The similar behaviors of optical activity for the organic chiral molecules in solutions were hold in solid gels. The specific rotations for C6H12O6 and C17H17ClO6 in gels were −0.95 and −1.45°/cm, corresponding to the chiral parameter 1.55 × 10−7 and 2.37 × 10−7, respectively.  相似文献   

7.
The low-temperature co-fired ceramic (LTCC) composites containing quartz based on the eutectic system BaO–Al2O3–SiO2–B2O3 are fabricated at the sintering temperature below 980 °C. Preparation process and sintering mechanism were described and discussed, respectively. The results indicated that the addition of quartz to the eutectic system can availably improve dielectric properties of the LTCC composites. In addition, The LTCC composites with optimum compositions, which were obtained by the regulation of an Al2O3 content in the composite, can express excellent dielectric properties (permittivity: 5.94, 5.48; loss: 7 × 10−4, 5 × 10−4), considerable CTE values (11.7 ppm. °C−1, 10.6 ppm. °C−1) and good mechanical properties (128 MPa,133 MPa).  相似文献   

8.
Nanocrystalline LaFeO3 was synthesized by calcining precursor La2(CO3)2(OH)2–Fe2O3?1.5H2O in air. XRD analysis showed that precursor dried at 80 °C was a mixture containing orthorhombic La2(CO3)2(OH)2 and amorphous Fe2O3?1.5H2O. Orthorhombic LaFeO3 with highly crystallization was obtained when La2(CO3)2(OH)2–Fe2O3?1.5H2O was calcined at 900 °C in air for 2 h. Magnetic characterization indicated that the calcined product at 900 °C behaved weak magnetic behavior at room temperature. The thermal process of La2(CO3)2(OH)2–Fe2O3?1.5H2O experienced five steps, which involves, at first, dehydration of 0.8 absorption water, then dehydration of 0.7 crystal water, decomposition of orthorhombic La2(CO3)2(OH)2 into orthorhombic LaCO3OH, reaction of two LaCO3OH into hexagonal La2O2CO3 and crystallization of tetragonal Fe2O3, at last, reaction of hexagonal La2O2CO3 with tetragonal Fe2O3 into orthorhombic LaFeO3. In the DTG curve, four DTG peaks indicated the precursor experienced mass loss of four steps.  相似文献   

9.
The density and volume fraction of an adsorbed phase of carbon dioxide (CO2) in aerogels was investigated using a formalism based on independent measurements of neutron transmission and small-angle neutron scattering from fluid-saturated absorbers (Rother et al. J. Phys. Chem. C 111, 15736 (2007)). The range of excess fluid pressures (0 <  P <  8 MPa) and temperatures (T = 35°C and 80°C) corresponded to the supercritical regime above the critical temperature T C = 31.1°C and critical density ρ C = 0.468 g · cm−3 of the bulk fluid. The results demonstrate that a porous aerogel matrix works to create an adsorbed phase with liquid-like fluid densities reaching ~1.1 g · cm−3 and ~0.8 g · cm−3 at T = 35°C and 80°C, respectively. Thus, despite the fact that the density and volume fraction of the adsorbed fluid both decrease with temperature, the dense adsorbed phase is still present in the aerogel at temperatures far exceeding the T C. Heat treatment (“oxidation”) of the aerogel at 500°C for 2 h, which removes a significant fraction of the alkyl groups from the aerogel surface, has little effect on the adsorption properties. The observed reduction of the density and volume fraction of the adsorbed CO2 with temperature and its minor dependence on the surface modification are consistent with predictions of the pore-filling model.  相似文献   

10.
The formation of the nanostructured WC–10 wt% Co powder from WO3, Co3O4, and graphite is studied. The effects of the processing parameters of high-energy ball milling, reduction in H2 atmosphere, and carburization in Ar/CO atmosphere are investigated. The crystallite size of the as-synthesized WC is 30–40 and 40–50 nm for 900 and 1000 °C carburized powders, respectively. The powder is agglomerated with the size of the primary particles ranging from 50 to 700 nm. High-energy ball milling of WO3–Co3O4–C powder mixtures leads to finer particle and crystallite sizes with larger surface area. Such milled powders can be reduced to nanostructured W at 570 °C and carburized to form WC at temperatures as low as 900 °C. Crystal growth has taken place during carburization, particularly at 1000 °C, which results in the formation of truncated triangular prisms and nanoplates of WC at 1000 °C.  相似文献   

11.
Mixed oxides and pyrochlore-type materials based on the Sr, Ce, Sn, and Mn elements have been prepared by hydrothermal method using a mixture of nitrate salts at 200 °C for 40 h under N2 atmosphere. Two groups of solids were synthesized: (i) (SrxCe1?x)2Sn2Oδ (0.345  x  0.365) and (ii) (SrxCe1?x)2(SnyMn1?y)2Oδ (0.345  x  0.365, 0.385  y  0.395). The structure of the solids were studied by X-ray diffraction and the main crystal phases determined were SnO2, (SrCe)2Sn2O7 and a trace amount of CeO2 in group (i) and only SnO2 and CeO2 were detected in group (ii). The mixed oxides/stannate pyrochlore have been tested as catalyst for NO reduction with hydrocarbons (CH4, C2H4, and C3H6) in the presence of O2. The CeO2 containing stannate Sr2xCe2?2xSn2Oδ pyrochlore coexist with SnO2 (group (i)) was found to be the best for NO + C3H6 reaction giving very high N2 production at 350 °C in the presence of O2 and water vapor. SnO2 as well as CeO2 alone were also synthesized by the hydrothermal method and their NO reduction properties have been compared with those of the groups (i) and (ii).  相似文献   

12.

Zinc oxide (ZnO) thin films were grown at 70 °C by plasma-enhanced atomic layer deposition using H2O and O2 plasmas. Plasma oxidants were used in order to improve the ZnO crystallinity and optoelectronic properties, avoiding high-temperature synthesis. The deposition parameters were optimized to achieve saturation in each reaction step. X-ray photoelectron spectroscopy (XPS) reveals high purity of the obtained ZnO films. X-ray diffraction (XRD) measurements indicate that the grown layers are polycrystalline and that the H2O plasma synthesis leads to better crystallinity than the O2 plasma as inferred from the intensity of the (100) and (002) peaks. The films are with high optical transmission, ~90%, as inferred from UV–visible (UV–Vis) transmittance measurements, and optical band gaps of 3.22 and 3.23 eV for H2O and O2 plasma, respectively. Atomic force microscopy (AFM) indicates that the films are smooth, with an average roughness of ~?0.22 nm. The growth rate was found to be in the range of 1.2–1.4 Å/cycle. The XPS, XRD, UV–Vis, and AFM results prove the possibility to obtain high-quality ZnO films by O2 and H2O plasma processes at 70 °C with chemical, structural, and optical properties promising for flexible electronics. ZnO films were successfully deposited on polyethylene terephthalate substrates using the optimal conditions for H2O plasma process. No damage of the film surface or substrate was observed.

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13.
A homogeneous α-Al2O3 crystal membrane was fabricated by the sol–gel technique on 316L porous stainless steel (PSS) substrate with an average pore size of 1.0 μm. The preparation process was optimized by carefully choosing the binder, the concentrations of the casting solutions and the sintering temperatures of the membranes. Compared to methylcellulose and polyethylene glycol 20000, polyvinyl alcohol 1750 was found to be the most effective binder to fabricate a homogeneously structured Al2O3 membrane without defects. The concentration to prepare an uniform coverage membrane with a thickness of ~10 μm was 0.032 mol/L. When sintered at 1000 °C, γ-Al2O3 membrane with ~3 μm grains was obtained. When sintered at 1200 °C, γ-Al2O3 completely transformed into α-Al2O3 and the grains grew to ~5 μm. Accordingly, the process was applied to a bigger pore-sized PSS with an average pore size of 1.5 μm to fabricate an α-Al2O3 intermediate layer to initially modify its surface. A single α-Al2O3 crystal layer with a thickness of ~5 μm and an average pore size of 0.7 μm was achieved. Subsequently, TiO2, SiO2, and TiO2–SiO2 hybrid membranes were tried on the modified PSS. Defect-free microfiltration membranes with average pore sizes of ~0.3 μm were readily fabricated. The results indicate that the sol–gel method is promising to initially modify the PSS substrates and the sol–gel-derived α-Al2O3 crystal layer is an appropriate intermediate layer to modify the PSS and to support smaller grain-sized top membranes.  相似文献   

14.
Precursor of nanocrystalline LaMnO3 was synthesized by solid-state reaction at low heat using La(NO3)3·6H2O, MnSO4·H2O, and Na2CO3·10H2O as raw materials. XRD analysis showed that precursor was a mixture containing orthorhombic La2(CO3)3·8H2O and rhombohedral MnCO3. When the precursor was calcined at 800 °C for 2 h, pure phase LaMnO3 with rhombohedral structure was obtained. Magnetic characterization indicated that rhombohedral LaMnO3 behaved weak magnetic properties. The thermal process of the precursor experienced four steps, which involved the dehydration of crystallization water at first, and then decomposition of manganese carbonate into MnO2, and decomposition of La2(CO3)3 and MnO2 together into La2O2CO3 and Mn2O3, and lastly reaction of monoclinic La2O2CO3 with Mn2O3 and formation of rhombohedral LaMnO3. Based on the Kissinger equation, the value of the activation energy associated with the formation of rhombohedral LaMnO3 was determined to be 260 kJ mol?1. The value of the Avrami exponent, n, was equal to 1.68, which suggested that crystallization process of LaMnO3 was the random nucleation and growth of nuclei reaction.  相似文献   

15.
ABi2Nb2O9 (A = Ca2+, Sr2+, Ba2+) were prepared by using an aqueous solution method from the mixture of water-soluble M-EDTA (M = Ca2+, Sr2+, Ba2+), Bi-EDTA, Nb-tartarate and TEA as the starting materials. A black fluffy mass resulted on heating the solution mixture at ∼200 °C. X-ray powder diffraction (XRD) showed that a single phase with the layered perovskite structure was formed after calcining the black fluffy mass at 600 °C. No intermediate phase was found during heat treatment at and above 600 °C. The particle size obtained from TEM lay between 20 and 30 nm. Structural electron microscopy (SEM) revealed that the average grain size after sintering at 900 °C for 4 h ranges from 1.2 to 1.67 μm with a relative compact density of ≥90%. A comparative study on dielectric constant and corresponding tangent loss were carried out at 1 kHz, 100 kHz, 1 MHz, and 5 MHz from which the Curie temperature (T c) was found to be at 935, 450, and 170 °C with peak dielectric constants at 930, 595, and 545, respectively, for CBN (CaBi2Nb2O9), SBN (SrBi2Nb2O9), and BBN (BaBi2Nb2O9) measured at frequency 100 kHz with very low tangent loss.  相似文献   

16.
The Zn2SiO4 ceramics with the addition of BaO and B2O3 are fabricated by traditional solid-state preparation process at a sintering temperature of 900 °C. The introduction of BaO and B2O3 to the binary system ZnO-SiO2 is achieved by adding 10 and 20 wt. % flux BB to the mixed ZnO-SiO2 ceramic powders pre-sintered at 1,100 °C, respectively. The chemical composition of the flux BB (50 wt.%BaO-50 wt.% B2O3) is located at a liquid phase zone with a temperature range of about 869–900 °C in the binary diagram BaO-B2O3. In addition, the introduction of BaO and B2O3 to the binary system ZnO-SiO2 is also achieved by the means of a chemical combination of H2SiO3, H3BO3, ZnO and Ba(OH)2·8H2O, which can result in the formation of the hydrated barium borates with low melting characteristics. In turn, by the liquid sintering aid of the barium borate melts, the preparation process of the Zn2SiO4 ceramics can be further simplified. In the two preparation methods, the Zn2SiO4 ceramics with the 1.5–2.0 ZnO/SiO2 molar ratios and the addition of a 10 wt. % flux BB can show good dielectric properties whereas the bending strength mainly depends on the microstructure of the Zn2SiO4 ceramics and SiO2 content in the composition of the specimen.  相似文献   

17.
Fe2O3/MgO system was prepared by wet impregnation method followed by treatment with different amounts of Zr-dopant salt then heating at 500 and 700 °C. The dopant concentrations were 0.48, 0.95 and 1.4 mol% ZrO2. Pure and variously doped solids were characterized using XRD, N2-adsorption isotherms carried out at ?196 °C and catalytic decomposition of H2O2 in aqueous solution at 25–35 °C. The results revealed that the nanosized MgO phase was only detected in the diffractograms of pure and doped solids calcined at 500 °C. Heating pure and doped solids at 700 °C produced nanosized MgFe2O4 phase together with MgO phase. Pure and ZrO2-doped solids calcined at 500 and 700 °C are mesoporous adsorbents. The doping process brought about a measurable decrease in the SBET of Fe2O3/MgO system with subsequent increase in its catalytic activity. The catalytic activity of the investigated system toward H2O2 decomposition, expressed as reaction rate constant per unit surface area was found to increase as a function of dopant concentration. The maximum increase in the reaction rate constant per unit surface area measured for the reaction carried out at 30 °C attained 125% for the heavily doped samples. This significant increase was based on the catalytic activity of pure catalyst sample measured under the same conditions.  相似文献   

18.
Belt-like VO2(A) with a rectangular cross section (VA-RCS) was successfully synthesized using V2O5, H2C2O4·2H2O and H2O as the starting materials by a facile hydrothermal approach. Some synthetic parameters, such as, the reaction time, reaction temperature and concentration of H2C2O4·2H2O, were systematically investigated to control the fabrication of belt-like VA-RCS. The formation mechanism of belt-like VA-RCS was proposed. Subsequently, belt-like VO2(M) with a rectangular cross section (VM-RCS) was prepared by the irreversible transformation of VA-RCS at 700 °C for 2 h under the inert atmosphere. The phase transition temperature (Tc) of VA-RCS and VM-RCS was evaluated by DSC test. The optical switching properties of VA-RCS and VM-RCS were studied by the variable-temperature infrared spectra, and it was found that the as-obtained VA-RCS and VM-RCS could be used as the optical switching materials. Furthermore, the oxidation resistance properties of VA-RCS and VM-RCS were investigated by TGA, indicating that they have good thermal stability and oxidation resistance below 400 °C in air.  相似文献   

19.
A molecular porous material, MPM-2, comprised of cationic [Ni2(AlF6)(pzH)8(H2O)2] and anionic [Ni2Al2F11(pzH)8(H2O)2] complexes that generate a charge-assisted hydrogen-bonded network with pcu topology is reported. The packing in MPM-2 is sustained by multiple interionic hydrogen bonding interactions that afford ultramicroporous channels between dense layers of anionic units. MPM-2 is found to exhibit excellent stability in water (>1 year). Unlike most hydrogen-bonded organic frameworks which typically show poor stability in organic solvents, MPM-2 exhibited excellent stability with respect to various organic solvents for at least two days. MPM-2 is found to be permanently porous with gas sorption isotherms at 298 K revealing a strong affinity for C2H2 over CO2 thanks to a high (ΔQst)AC [Qst (C2H2) − Qst (CO2)] of 13.7 kJ mol−1 at low coverage. Dynamic column breakthrough experiments on MPM-2 demonstrated the separation of C2H2 from a 1:1 C2H2/CO2 mixture at 298 K with effluent CO2 purity of 99.995% and C2H2 purity of >95% after temperature-programmed desorption. C-H···F interactions between C2H2 molecules and F atoms of AlF63− are found to enable high selectivity toward C2H2, as determined by density functional theory simulations.  相似文献   

20.
Anodic alumina oxides (AAOs) prepared in oxalic acid (H2C2O4) solution at a constant voltage of 40 V were investigated by the techniques of temperature programmed desorption combined mass spectrograph (TPD-MS), thermogravimetric analysis (TGA), differential thermal analysis (DTA) and photoluminescence (PL). The results indicate that the desorption of H2O, CO and CO2 and the decomposition of H2C2O4 which led to the weight loss of AAOs samples occurred below 400 °C, while the water desorption was the main reason for weight loss. In the temperature range of 400–900 °C, a small quantity of aluminum oxalate (Al2(C2O4)3) decomposed and gave birth to CO and CO2, during this process CO became the major product. The drastic decompositions of aluminum carbonate (Al2(CO3)3) and Al2(C2O4)3 took place near 930 °C, which produced a large amount of CO2. The amount of (C2O4)2− embedded in bulk AAOs was calculated versus the total weight of AAOs film, and the PL intensity of AAOs was correlated to the doping of oxalic acid radical. The above results may have great significance in the better application of AAOs as matrix of photonic crystals.  相似文献   

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