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1.
Porous semiconducting (Ba, Sr)TiO3 ceramics were fabricated by the addition of potato-starch to the (Ba, Sr)TiO3 powders. The effects of potato-starch on the microstructure and PTCR characteristics of the porous (Ba, Sr)TiO3 ceramics have been investigated. The porosity largely increased and the grain size slightly decreased with increasing potato-starch content. The crystalline structure of (Ba, Sr)TiO3 ceramics was independent of the potato-starch content. The (Ba, Sr)TiO3 ceramics containing potato-starch showed higher PTCR (106) characteristics than that of the (Ba, Sr)TiO3 ceramics without potato-starch. It was found that the development of PTCR characteristic in the porous (Ba, Sr)TiO3 ceramics containing various amounts of potato-starch, in the same way as normal BaTiO3 ceramics without potato-starch, is associated with grain boundaries, from the impedance analysis.  相似文献   

2.
Rutile TiO2 (a=4.594 å and c=2.958 å) phase was formed on the outer region of Ti powders after oxidation at 600 °C for 1–300 h. Porous (Ba,Sr)TiO3 ceramics were fabricated by adding partially oxidized Ti powders (4–8 vol %) into (Ba,Sr)TiO3 powders, and showed excellent positive temperature coefficient of resistivity (PTCR) characteristics after paste-baking treatment at 580 °C in air. The PTCR characteristics of the porous ceramics were mainly attributed to the adsorption of oxygen at the grain boundaries. The microstructure and electrical properties of the porous (Ba,Sr)TiO3 ceramics containing the partially oxidized Ti powders oxidized at 600 °C for different oxidation times (1–300 h) were investigated.  相似文献   

3.
Porous Ba(Ti,Sb)O3 ceramics were fabricated by adding corn-starch at 20 wt %. The effect of atmosphere on the PTCR characteristics of the porous Ba(Ti,Sb)O3 ceramics and the role of oxygen on the grain boundaries in the PTCR characteristics of the Ba(Ti,Sb)O3 ceramics were investigated. In air, O2, N2, and H2 atmospheres, the electrical resistivity of Ba(Ti,Sb)O3 ceramics below 150 °C was independent of atmosphere, while it was strongly dependent on atmosphere above 200 °C. The low electrical resistivity in reducing atmospheres was due to a decrease in potential barrier height, which originated from an increase in the number of electrons owing to the desorption of chemisorbed oxygen atoms at the grain boundaries. In a N2 atmosphere, the electrical resistivity of Ba(Ti,Sb)O3 ceramics during the cooling cycle was lower than that during the heating cycle, and then the electrical resistivity of the porous Ba(Ti,Sb)O3 ceramics during subsequent heating and cooling cycles was increased again by exposure to an O2 atmosphere.  相似文献   

4.
An approach is proposed for fabricating fine-grained, low-resistivity BaTiO3-based PTCR ceramics via partial isovalent substitutions on the Ba site. The grain size of the ceramics thus prepared is shown to decrease as the ratio of ionic radii r(Ba2+)/r(M2+) (M = Ca, Sr, Pb) increases. Isovalent substitutions on the Ba site narrow down the range of donor dopant (yttrium) concentrations in which PTCR materials can be prepared. The experimental results agree well with thermodynamic calculations under the assumption that the materials contain the Y3+Ti3+O3 phase, as suggested by ESR data, which point to the presence of Y3+–Ti3+ associates. Partial calcium, strontium, and lead substitutions on the Ba site reduce the average grain size of PTCR ceramics, which is probably due to the lattice strain arising from the isovalent substitution. Partial replacement of Ba2+ with mixtures of different isovalent elements (e.g., Sr2+ and Pb2+) offers the possibility of obtaining fine-grained, low-resistivity PTCR ceramics, without changing the phase transition temperature.  相似文献   

5.
The (Ba,Sr)TiO3 amorphous gel was prepared by sol-gel process and calcined in the 2.45-GHz multimode microwave furnace to synthesize (Ba,Sr)TiO3 nanopowder. The calcination temperature of the (Ba,Sr)TiO3 ceramic powders that convert the material into prevoskite phase can be reduced from 1100°C to 900°C, the nanopowder displays the highest sinterability. Using a new kind of insulator materials made of MgAl2O4–LaCrO3, the crack-free and dense (Ba0.80Sr0.20)TiO3 ceramics with fine grain size (<1 µm) were prepared by microwave sintering at 1310°C for 15 min. The fine (Ba,Sr)TiO3 ceramics sintered by microwave sintering technique display lower dielectric loss than that of conventional samples, indicating a reduction of the influence of defects with the microwave process.  相似文献   

6.
《Materials Letters》2007,61(4-5):1007-1010
Sb2O3-doped Ba0.672Sr0.32Y0.008TiO3 (BSYT) dielectric ceramics were prepared by conventional solid state method, and their dielectric properties were investigated with variation of Sb2O3 doping content and sintering temperature. The X-ray diffraction patterns indicated that all the BSYT specimens possessed the perovskite polycrystalline structure. The experimental results reveal that the introduction of Sb2O3 into Ba0.672Sr0.32Y0.008TiO3 can control the grain growth, reduce the relative dielectric constant and dielectric loss, shift the Curie temperature to lower temperature and significantly improve the thermal stability of the BSYT ceramics. The samples doped with 1.6 wt.% Sb2O3 sintered at 1320 °C for 2 h exhibited attractive properties, including high relative dielectric constant (> 1500), low dielectric loss (< 40 × 10 4), low temperature coefficient of capacitor(< ± 35%) over a wide temperature range from − 25 °C to + 85 °C.  相似文献   

7.
Lead-free PTCR ceramics based on Bi2O3 and Y2O3 doped Ba0.95Ca0.05TiO3 were fabricated by the conventional mixed oxide method, while Bi2O3 and Y2O3 were doped directly or after pre-calcining, in the molar ratio of Bi2O3:Y2O3 = 1:1. There were two synthesizing route, i.e. the materials were pre-calcined at 900 °C to obtain BiYO3 firstly and then doped into the basic materials, and the materials were directly doped into the starting materials, both of which could obtain samples with different electrical properties and PTCR behavior. The samples were characterized by using X-ray diffraction, scanning electron microscope, dielectric constant-temperature and resistivity-temperature measurement instrument. It was revealed that the perovskite lattice, the microstructure and the PTCR behavior of Ba0.95Ca0.05TiO3 varied with different doping contents and methods. A further research was conducted so as to study the electrical properties of ceramics by impedance spectroscopy.  相似文献   

8.
Porous n-BaTiO3 ceramics are synthesized by the addition of pore-forming agent into the (Ba,Sr)TiO3 powder. From the DTA-TGA analysis for samples containing the PEG and corn-starch, it was found that an exotherm occurred at 262 and 315°C, respectively, weight loss commenced at 165 and 252°C, and was virtually complete by 265 and 472°C, respectively. The porosity of n-BaTiO3 ceramics increased and the grain size decreased with increasing the pore-forming agent. From the XRD analysis at high angles, all the samples with and without the pore-forming agent at room-temperature exhibit the tetragonal structure. PTCR jump of the samples containing pore-forming agent is 1-2 orders higher than that of sample without the pore-forming agent. It is also found that the development of PTCR characteristic in the porous n-BaTiO3 ceramics containing pore-forming agent is related to grain boundaries, which basically equals that in ordinary BaTiO3 without pore-forming agent, from the complex impedance results.  相似文献   

9.
The Sr and Ca added to BaTiO3 in order to shift transition temperature near room temperature. The donor (Yb2O3) and acceptor (MnCO3) impurities were added to the (Ba,Sr,Ca)TiO3 powder for the improvement of structural and electrical properties. The (Ba,Sr,Ca)TiO3 powder was made by sol-gel method and the thick films were fabricated by screen-printing. We fabricated array type thick films. The 1 mm × 3 mm array thick films were arranged 2 × 8. Relative dielectric constant and dielectric loss of Yb2O3 0.1 mol% doped (Ba,Sr,Ca)TiO3 array thick film were 1068 and 2.8%, respectively at Curie temperature, 44 °C. Pyroelectric coefficient and F.M.D* showed 21.7 × 10−9 C/cm2 K and 3.2 × 10−9 C cm/J, respectively.  相似文献   

10.
The secondary phase compositions in Sb-doped (Ba, Sr)TiO3 ceramics containing SiO2 and excess TiO2 sintering additives have been examined by XRD, BEI and EPMA techniques. It is shown that alongside the primary (Ba0.797Sr0.2Sb0.003)TiO3 phase, (Ba1.95Sr0.05)2(Ti1.2Si1.8)O8 and Sb-doped (Ba0.99Sr0.01)6Ti17O40 phases form at the intergranular regions. Substitution of up to 0.04 mol% MnO2 enhances the PTCR effect, giving a ratio ρmaxmin ∼ 7 × 105 for the optimum 0.04% MnO2 composition. At this level Mn cannot be detected in the microstructure by EPMA, however in insulating samples containing 0.08 mol% of MnO2, it was detected in the (Ba0.99Sr0.01)6Ti17O40 intergranular phase.  相似文献   

11.
Processing characteristics of PTCR ceramics with low sintering temperature   总被引:2,自引:0,他引:2  
The processing behavior of PTCR ceramics of (Ba,Sr,Ca,Pb)TiO3 solid solution composition with additives of lanthanum oxide (La2O3) and boron nitride (BN) was studied. The ceramics can be sintered at temperatures as low as 1100 °C and possess rather low room-temperature resistivity with good PTCR effect. The sample ball milled with de-ionized water exhibits a more uniform microstructure compared to the sample ball-milled with alcohol. Particle size of less than 1 m was found to be adequate for preparing the ceramics and the finer particles (0.45 m) do not significantly improve the PTCR behavior. The performance of the PTCR sample is not sensitive to the sintering parameters such as the sintering time and cooling rate. This may be ascribed to the presence of excess BaO in the sample and the low sintering temperature, thereby eliminating the effect of Ba ion vacancies on the properties of the PTCR sample.  相似文献   

12.
The influence of B2O3, and Al2O3 as segregative additives in modifying the ρ–T characteristics has been studied in BaTiO3 ceramics with positive temperature coefficient of resistance (PTCR). Reaction of Al2O3 at the grain boundary regions of BaTiO3 ceramics leads to the segregation of the secondary phase, BaAl6TiO12 resulting in broad PTCR jump, whereas B2O3 addition gives rise to steeper resistivity jump. Microstructure studies by SEM reveal the formation of coherent second phase layer of barium aluminotitanate surrounding the BaTiO3 grains. The EDX results shows varying Al to Ti ratio in the early stage of phase formation in BaAl6TiO12 resulting in electrically active layer around the BaTiO3 grains. The TiO2-excess melt formation results in lower resistivity for 2–4% Al2O3 containing n-BaTiO3 ceramics whereas at higher alumina contents, BaAl6TiO12 phase becomes dominant leading to higher resistivity in the sample. Complex impedance analyses support the three-layer regions, corresponding to the contributions from grain interior resistance (R g), grain boundary resistance (R gb), and that from secondary phase (R sec). Electron paramagnetic resonance spectroscopy (EPR) indicated barium vacancies, V Ba / as the major electron trap centers which are activated across the tetragonal-to-cubic phase transition. A charge trapping mechanism is proposed wherein the segregation of secondary phases bring carrier redistribution among the various acceptor states thereby affecting the electrical conductivity of n-BaTiO3 ceramics. The presence of Al3+–O–Al3+ or Ti4+–O–Al3+ type hole centers at the grain boundary layer (GBL) regions results in charge redistribution across the modified phase transition temperature due to symmetry-related vibronic interactions resulting in broad PTCR characteristics extending to higher temperatures.  相似文献   

13.
蒸汽掺杂-一种新的钛酸钡基PTCR陶瓷的掺杂方法   总被引:4,自引:0,他引:4  
晶界铲应是陶瓷材料所固的的特性,利用某些氧化物在高温下具有较高的蒸汽压,在烧成过程对陶瓷材料进行掺杂改性,可以有效地控制晶界行为,改善材料性能,钛酸钡基半导体陶瓷中存在的PTCR效应,是一种典型的晶界效应。  相似文献   

14.
The grain growth kinetics in the 0, 2 and 4 wt.% TiO2 added ZnO–6 wt.% Bi2O3 system was studied using the simplified phenomenological grain growth kinetics equation together with the physical properties of the sintered samples. The grain growth exponent value (n) and the apparent activation energy for the ZnO–6 wt.% Bi2O3 system was 5 and 218 kJ/ mol, respectively. The addition of the TiO2 to the ZnO–6 wt.% Bi2O3 system inhibited the ZnO grain growth. At 2 and 4 wt.% TiO2 additions, the apparent activation energies were calculated as 467 and 346 kJ/ mol, respectively. The addition of TiO2 to the system inhibited the grain growth of ZnO ceramics.  相似文献   

15.
Two newly synthesised Sr0.50SbFe(PO4)3 [Sr0.5.] and SrSb0.50Fe1.50(PO4)3 [Sr.] phases were obtained by conventional solid-state reaction techniques at 1000 °C in air atmosphere. Their crystallographic structures were determined at room temperature from X-ray powder diffraction (XRPD) data using the Rietveld analysis. Both compounds belong to the Nasicon structural family. [Sr0.5.] and [Sr.] crystallise in rhombohedral system with \textR[`3] {\text{R}}\overline{3} and \textR[`3] \textc {\text{R}}\overline{3} {\text{c}} space group, respectively. Hexagonal cell parameters for [Sr0.5.] and [Sr.] are: a = 8.227(1) ?, c = 22.767(2) ? and a = 8.339(1) ?, c = 22.704(2) ?, respectively. Sr2+ and vacancies in {[Sr0.50]3a[□0.50]3b}M1SbFe(PO4)3 are practically ordered within the two positions, 3a and 3b, of M1 sites. Structure refinements show also an ordered distribution of Sb5+ and Fe3+ ions within the Nasicon framework. Within the structure, each Sr(3a)O6 octahedron shares two faces with two Fe3+O6 octahedra and each vacancy (□(3b)O6) site is located between two Sb5+O6 octahedra. In [Sr]M1Sb0.50Fe1.50(PO4)3 compound, all M1 sites are occupied by Sr2+ and the Sb5+ and Fe3+ ions are randomly distributed within the Nasicon framework. A Raman and infrared spectroscopic study was used to obtain further structural information about the nature of bonding in both selected compositions.  相似文献   

16.
The electrical properties and microstructure of (Ba,Y)TiO3 PTCR ceramics were studied. The results indicate that the Mn ions increase the intergranular barrier height and produce a high-resistance layer on the grain surface. The temperature-dependent resistances of the grain bulk, surface layer, and grain boundaries, the temperature coefficient of resistance, and the magnitude of the varistor effect were assessed as a function of Mn content.  相似文献   

17.
In this work, self-assembled monolayers (SAMs) of octadecyltrichlorosilane (OTS) were applied to induce the nucleation and growth of the antimony sulfide (Sb2S3) films on the functional ITO glass substrate at low temperature. The structure, morphology, and optical properties of the Sb2S3 films were investigated by X-ray diffraction, scanning electron microscopy, X-ray energy dispersive spectroscopy, and UV–vis spectroscopy. After thermal treatment at 200 °C for 1 h in air, the orthorhombic Sb2S3 was formed as a predominant phase in the deposited thin films. When the deposited films were thermally treated at 400 °C for 1 h in air, the orthorhombic Sb2S3 was decomposed and a cubic Sb2O3 was formed. The optical band energies of the as-deposited and thermally treated Sb2S3 films at 200 °C for 1 h in air and nitrogen were found to be 2.05 eV, 1.77, and 1.76 eV, respectively. As chemical templates, the OTS-functionalized SAMs played an important role in controlling the nucleation and growth of Sb2S3 films at low temperature. The results obtained from different preparation parameters applied in the present work will allow controlling the growth of the Sb2S3 films with uniform surface.  相似文献   

18.
《Materials Letters》2006,60(17-18):2059-2065
Thin films of (Bi0.5Sb0.5)2Te3 of different thickness were deposited on glass substrate by the flash evaporation method in a vacuum of 1 × 10 5 Torr. X-ray diffraction and transmission electron microscope analysis indicates that these films are polycrystalline even in the as-deposited state and the post-deposition annealing leads to grain growth. Electrical resistivity studies were carried out on these films as a function of temperature (300– 450 K) and film thickness (450–2000 Å). Temperature dependence of electrical resistivity shows that (Bi0.5Sb0.5)2Te3 films are semiconducting. It is found that electrical conduction activation energy decreases with increase of film thickness and this observation is explained based on the Slater model. Thickness dependence of electrical resistivity is analyzed using the effective mean free path model of size effect with perfect diffuse scattering. This analysis leads to the evaluation of the important physical parameters i.e., mean free path and bulk resistivity of hypothetical bulk.  相似文献   

19.
Nonstoichiometric BaTiO3 PTCR type materials are investigated with various amounts of MnO2, Sb2O3 and MgO dopants. Specimens fired with a nonisothermal rate-controlled sintering profile exhibit a rather fine and uniform microstructure as compared to those processed by conventional sintering techniques. The temperature at which the resistivity anomaly begins is observed to decrease with Sb2O3 and MgO contents. The Curie point of BaTiO3-based ceramics can be altered by addition of Sb2O3, and the dielectric peak is maintained by the presence of MgO additive. Magnesium ions act as acceptors in the BaTiO2 lattice, while antimony ions as donors. The presence of magnesium compensates some of the antimony, hence the doped-BaTiO3 seminonductive region is pushed to higher contents.  相似文献   

20.
The effects of SiO2 and Cr2O3 on the formation process of ZnO varistors were investigated. Prior to formation of the Zn2.33Sb0.67O4 spinel phase (Sp-phase), a spinel-like phase forms. However, this phase does not control the varistor microstructure. The Sp-phase and the Bi2O3-phase which were formed by the decomposition of the Bi2(Zn4/3Sb2/3)O6 pyrochlore phase played important parts in the control of the varistor microstructure. That is, the Bi2O3 phase produced in the reaction promotes the initial sintering of the varistor and the Sp-phase inhibits the ZnO grain growth. In this reaction, SiO2 and Cr2O3 play a role in decreasing the decomposition temperature of the pyrochlore phase. Decreasing the decomposition temperature below 900° C (where ZnO grain growth begins) leads to the inhibition of ZnO grain growth.  相似文献   

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