锰掺杂Bi0.5Na0.41K0.09TiO3+xMnO2陶瓷的电学性能

采用传统陶瓷工艺、按照Bi0.5Na0.41K0.09TiO3+xMnO2的配方进行称量,其中x=0、0.005、0.01、0.03、0.05,共5个组分,制备出了无铅压电陶瓷坯体,在其烧结温度下进行烧结,制备了新型压电陶瓷Bi0.5Na0.41K0.09TiO3+xMnO2,并研究了该体系陶瓷的电学性能,测试其压电常数(d33)、机电耦合系数(Kp)、机械品质因素(Qm)、介电常数(εr)、介质损耗Tanδ及其电滞回线,并分析掺杂量对其性能的影响。     

Al2O3掺杂对Cu3Ti2Ta2O12陶瓷微观结构及介电性能的影响

采用固相反应法制备了Al₂O₃掺杂Cu₃Ti₂Ta₂O₁₂ (CTTAO)陶瓷,研究了其晶相组成、微观结构、复阻抗及介电性能。研究结果表明：CTTAO陶瓷样品为立方类钙钛矿结构,空间群Im3。随着Al₂O₃掺量的增加,样品的平均晶粒尺寸、介电系数和介电损耗均先减小后增大。结合复阻抗谱分析表明,CTTAO陶瓷具有半导性晶粒和绝缘性晶界构成的非均匀性微观结构,低频下的介电损耗主要由晶界电阻决定,利用内部阻挡层效应(IBLC)和MaxwellWagner极化弛豫模型,可解释CTTAO的巨介电响应。     

Bi2O3对K2O–B2O3–SrO–Al2O3–Nb2O5–SiO2玻璃陶瓷介电储能性能的影响

随着电力电子系统的不断发展,高功率脉冲电容器的需求增多。电介质电容器因具有放电功率大、充放电速度快及性能稳定等优点,在电力系统、电子器件、脉冲电源等方面发挥着重要作用,广泛应用于民用领域及军事领域。通过熔融压延制备玻璃基体,采用可控结晶工艺研究了不同含量的Bi₂O₃ (x=0.0%、1.0%、2.0%、4.0%,摩尔分数)对K₂O–B₂O₃–Sr O–Al₂O₃–Nb₂O₅–SiO₂玻璃陶瓷物相演化、微观结构、介电和储能性能的影响。在该玻璃陶瓷中,KSr₂Nb₅O₁₅为主要析出晶相,当Bi₂O₃的加入量为x=2.0%(摩尔分数)时,热处理温度为950℃时,玻璃陶瓷样品的储能密度最大可达到1.27 J/cm³,室温下介电常数可达342,是热处...     

Ni掺杂对BaTiO3陶瓷物相及介电性能的影响

采用固相反应法制备了BaTi_1-xNi_xO₃（x=0、0.01、0.05、0.08、0.1、0.2）陶瓷,研究了不同Ni掺杂量对BaTi_1-xNi_xO₃陶瓷的相结构和介电性能的影响。采用X射线衍射技术（XRD）分析了BaTi_1-xNi_xO₃陶瓷的相结构;采用阻抗分析仪测试BaTi_1-xNi_xO₃陶瓷介电性能。XRD分析结果表明:随着Ni的掺杂量的增加,BaTi_1-xNi_xO₃陶瓷的晶相由四方相逐渐转变为六方相,当Ni的掺杂量为x=0.1时,BaTi_1-xNi_xO₃完全变为六方相。随着Ni含量的增大,所有六方相的BaTi_1-xNi_xO₃的晶格常数都变大,且相对介电常数ε_r整体降低而介电损耗tanδ呈现先减小后增大的趋势。     

铁钕掺杂K0.5Na0.5NbO3陶瓷的压电介电性能

采用传统陶瓷制备技术制备了新型的K0.5Na0.5NbO3+0.2%molFe2O3+x%molNd2O3压电陶瓷,研究了该体系陶瓷的压电性能及介电性能。研究结果表明,在烧结温度为1120℃、4 h时,该体系陶瓷均具有相对较好的电学性能,并在x为0.2时性能最佳,其压电常数d33为125pC/N,机电耦合系数Kp为37%,机械品质因素Qm为155,介电常数εr为561,介质损耗tanδ为0.08。     

离子对(Nb5+-Cr3+)掺杂对0.93Bi0.5Na0.5TiO3-0.07BaTiO3陶瓷微观结构和电学性能的影响

采用固相烧结法制备(Bi0.5Na0.5)0.93Ba0.07Ti1-x(Nb0.5Cr0.5)xO3(摩尔分数x=0％、0.5％、1％、2％、2.5％、5％)(简称BNBT-xNC)无铅压电陶瓷,研究离子对(Nb5+-Cr3+)对0.93Bi0.5Na0.5TiO3-0.07BaTiO3(简称BNT-7BT)陶瓷微观...     

Effect of Doping Eu on the Electrical and Magnetic Properties of Bi5Fe0.sCo0.5Ti5O15 Ceramics

用传统固相烧结法制备了 Bi5–xEuxFe0.5Co0.5Ti3O15（BEFCT–x：x = 0,0.35,0.55,0.85）陶瓷样品,对比研究了它们的结构和电磁性能。X 射线衍射分析表明：掺杂未导致明显杂相,材料的剩余极化（2Pr）随掺杂量的增加呈先增加后减小的变化趋势,在 Eu 掺杂量为 0.55 时,材料的 2Pr达到最大值,为 11.2μC/cm2,升幅达 143%,可以由 Eu 掺杂导致氧空位的抑制和铋氧层的破坏所形成的竞争机制解释。随 Eu 含量的增加,材料的剩余磁化单调上升,最大达到 0.28 A m2/kg,比未掺杂时增加了 2 个数量级,从晶格失配、耦合增强以及共生结构等方面的综合效果解释了这一现象。材料的介电温度谱显示,Eu 掺杂未明显损害材料的热稳定性,Eu 掺杂所导致的介电损耗行为可能与氧空位或其他点缺陷有关联。     

烧结温度对Y3+掺杂Ba0.62Sr0.38TiO3陶瓷介电性能的影响

采用固相合成法,以BaCO3、SrCO3和TiO2等为原料,Y2O3为掺杂剂,制得了Ba0.62Sr0.38TiO3系介质瓷,研究了烧结温度对体系介电性能的影响。结果表明:随着烧结温度的升高,试样的体积密度在1300℃时出现一个极大值,达到5.353g/cm3,之后随温度继续升高略有减小,而试样的气孔率随烧结温度的变化则与之相反,且在1300℃时达到极小值1.54%;试样的介电峰值先升高后下降,在1280℃时达到最大值,与此同时,试样Tm移向低温方向,Tm的这种变化与试样的晶粒尺寸略有增大,以及Y3+更容易进入晶格B位位置有关。     

Nd2O3掺杂对BCZT陶瓷结构及介电性能的影响

采用固相反应法制备Ba0.92-xCa0.08Ndx(Zr0.18Ti0.815Y0.0025Mn0.0025)O3(BCZT-Nd,x=0、0.005、0.010、0.020)陶瓷,研究了Nd2O3掺杂对Ba0.92Ca0.08(Zr0.18Ti0.82)O3(BCZT)陶瓷结构及介电性能的影响。结果表明,不同含量Nd3+作为施主掺杂离子进入A位和含量均为0.25%(摩尔分数)的Mn2+和Y3+作为受主掺杂进入B位均能提高BCZT陶瓷的致密性,细化晶粒作用明显,所有样品均为单一的四方BaTiO3相结构。随Nd2O3掺杂量增加,BCZT-Nd陶瓷介电峰值温度Tm向低温方向移动,相变弥散程度增强,Nd3+含量≥0.005mol时即表现出明显的弛豫铁电体特征。     

Nb5+掺杂改性CaBi4Ti4O15压电陶瓷的研究

采用传统固相烧结法,制备了CaBi4Ti(1-x)NbxO1(5x=0.00-0.05,CBT-N)系铋层状结构无铅压电陶瓷。研究了Nb5+掺杂对CBT压电陶瓷压电与介电性能的影响。研究结果表明:添加Nb5+离子,改善了CBT陶瓷的烧结特性,提高了瓷体的致密度。Nb2O5的引入降低了CBT系列陶瓷的介质损耗,改善了陶瓷的压电与介电性能。当掺入量x=0.04(CaBi4Ti0.96Nb0.04O15)时制备的CBT基铋层状压电陶瓷具有优异的压电性能:d33=14pC/N,Qm=3086,εr=212,tanδ=0.0041,kt/kp=1.681。     

Effect of Bi2O3 and B2O3 additives on the sintering temperature, microstructure, and microwave dielectric properties for Sm(Mg0.5Ti0.5)O3 ceramics

The microwave dielectric properties of Sm(Mg_0.5Ti_0.5)O₃ incorporated with various amount of Bi₂O₃ and B₂O₃ additives have been investigated systematically. In this study, both Bi₂O₃ and B₂O₃ additives acting as a sintering aid can effectively lower the sintering temperature from 1550 °C to 1300 °C. The ionic radius of Bi³⁺ for a coordination number of 6 is 0.103 nm, whereas the ionic radius of B³⁺ is 0.027 nm. Clearly, the ionic radius of Bi³⁺ is greatly larger than one of B³⁺, which resulted in the specimens incorporated with Bi₂O₃ having larger lattice parameters and cell volume than those incorporated with B₂O₃. The experimental results show that no second phase was observed throughout the entire experiments. Depending on the interfacial tension, the liquid phase may penetrate the grain boundaries completely, in which case the grains will be separated from one another by a thin layer as shown in Sm(Mg_0.5Ti_0.5)O₃ ceramics incorporated with Bi₂O₃. Whereas, in Sm(Mg_0.5Ti_0.5)O₃ ceramics incorporated with B₂O₃, the volume fraction of liquid is high, the grains may dissolve into the liquid phase, and rapidly rearrange, in which case contact points between agglomerates will be dissolved due to their higher solubility in the liquid, leading plate-like shape microstructure.A dielectric constant (?_r) of 29.3, a high Q × f value of 26,335 GHz (at 8.84 GHz), and a τ_f of −32.5 ppm/°C can be obtained for Sm(Mg_0.5Ti_0.5)O₃ ceramics incorporated with 10 mol% Bi₂O₃ sintered at 1300 °C. While Sm(Mg_0.5Ti_0.5)O₃ ceramics incorporated with 5 mol% B₂O₃ can effectively lower temperature coefficient of resonant frequency, which value is −21.6 ppm/°C. The Sm(Mg_0.5Ti_0.5)O₃ ceramic incorporated with heavily Bi₂O₃ and B₂O₃ additives exhibits a substantial reduction in temperature (∼250 °C) and compatible dielectric properties in comparison with that of an un-doped one. This implied that this ceramic is suitable for miniaturization in the application of dielectric resonators and filters by being appropriately incorporated with a sintering aid.     

SrCO3掺杂对BMT陶瓷结构及介电性能的影响

采用固相烧结法制备SrCO3掺杂Ba（Mg1/3Ta2/3）O3（BMT）微波介质陶瓷,研究SrCO3质量（下同）掺量w（SrCO3）=2%～8%对BMT微波介质陶瓷结构和介电性能的影响。结果表明：添加适量SrCO3可以促进烧结并在一定程度上提高BMT陶瓷体系的B位离子1：2有序度;当w（SrCO3）=6%时,陶瓷致密...     

Effect of Bi2O3 additives on sintering and microwave dielectric behavior of La(Mg0.5Ti0.5)O3 ceramics

Bi₂O₃ was selected as liquid phase sintering aid to lower the sintering temperature of La(Mg_0.5Ti_0.5)O₃ ceramics. The sintering temperature of La(Mg_0.5Ti_0.5)O₃ ceramics is generally high, about 1600 °C. However, the sintering temperature was significantly lowered about 275 °C from 1600 °C to 1325 °C by incorporating in 15 mol% Bi₂O₃ and revealed the optimum microwave dielectric properties of dielectric constant (?_r) value of 40.1, a quality factor (Q × f) value of 60,231 GHz, and the temperature coefficient (τ_f) value of 70.1 ppm/°C. During all addition ranges, the relative dielectric constants (?_r) were different and ranged from 32.0 to 41.9, the quality factors (Q × f) were distributed in the range of 928–60,231 GHz, and the temperature coefficient (τ_f) varies from 0.3 ppm/°C to 70.3 ppm/°C. Noticeably, a nearly zero τ_f can be found for doping 5 mol% Bi₂O₃ sintering at 1325 °C. It implies that nearly zero τ_f can be achieved by appropriately adjusting the amount of Bi₂O₃ additions and sintering temperature for La(Mg_0.5Ti_0.5)O₃ ceramics.     

Composite cathodes of La0.9Ca0.1Ni0.5Co0.5O3-Ce0.8Sm0.2O1.9 for solid oxide fuel cells

The mixed ionic and electronic conductors of La_0.9Ca_0.1Ni_0.5Co_0.5O₃-Ce_0.8Sm_0.2O_1.9 (LCNC-SDC) are investigated systematically for potential application as a cathode for solid oxide fuel cells based on a Ce_0.8Sm_0.2O_1.9 (SDC) electrolyte. The electrochemical impedance spectroscopy (EIS) measurements are performed in air over the temperature range of 600-850 °C to determine the cathode polarization resistance. The exchange current densities for oxygen reduction reaction (ORR), determined from the low-field cyclic voltammetry, high-field cyclic voltammetry, and EIS data are systematically investigated. The activation energies (E_a) for ORR determined from the slope of Arrhenius plots are in the range of 102.33-150.73 kJ mol⁻¹ for LCNC-SDC composite cathodes. The experimental results found that LCNC-SDC (70:30) composite cathode has a maximum exchange current density and a minimum polarization resistance of 0.30 Ω cm² for 850 °C among LCNC-SDC composite cathodes.     

Dielectric,magnetic and magnetoelectric properties of Ni0.5Zn0.5Fe2O4+Pb(Zr0.48Ti0.52)O3 composite ceramics

Magnetoelectric composite ceramics of spinel ferrite Ni_0.5Zn_0.5Fe₂O₄ (NZFO) with high magnetic permeability and tetragonal perovskite Pb(Zr_0.48Ti_0.52)O₃ (PZT) with high piezoelectric constant were synthesized by common solid state reaction method. XRD and SEM showed that high dense composite ceramics without any foreign phases were obtained. The ceramics showed excellent dielectric and magnetic properties, which were stable in a large frequency range. The dielectric peak became wider with the ferrite content in the permittivity spectrum with temperature. With the increase in the ferrite content, the magnetic Curie temperature shifted to higher temperature and closed to that of the pure ferrite. In addition, the magnetoelectric coefficient enhanced as the increase in the ferrite content. The properties of the composite ceramics could be adjusted by the ferrite content. These research results provided a powerful experimental basis for the sensor and transducer in microelectronic and microwave devices.     

Structural and electrical properties of La0.7Sr0.3Co0.5Fe0.5O3 powders synthesized by solid state reaction

This work investigates the effect of synthesis parameters (calcination temperature, milling conditions and sintering temperature) on the structural, morphological and electrical properties of La_0.7Sr_0.3Co_0.5Fe_0.5O₃ (LSCF) powders prepared by the solid state reaction. The thermogravimetric profile showed that the minimum temperature needed for the carbonate decomposition and formation of perovskite phase is 800 °C. SEM analysis revealed the loose and porous structure of the powder materials. The XRD patterns demonstrate that milling parameters such as grinding balls:sample ratio, rotational speed, and milling time influence the structural properties. The results revealed that powders synthesized with grinding balls:sample ratio of 8:1, 500 rpm and 4 h of milling present pure LSCF phase. Porosity of the pellets decreased with increasing sintering temperature from 950 to 1100 °C. Electrical conductivity was measured at 400–1000 °C and correlated with sintering temperature.     

Electrical properties of niobium doped Bi4Ti3O12-SrBi4Ti4O15 intergrowth ferroelectrics

Nb-doped Bi₄Ti₃O₁₂-SrBi₄Ti₄O₁₅ intergrowth ceramics have been prepared by modified oxalate route. XRD phase analysis confirmed the formation of single phase compound. Nb-doping does not affect the basic crystal structure of the intergrowth. SEM micrographs showed that the grain size of the ceramics decreases with Nb-doping. The temperature dependence of dielectric constant and losses was investigated in the temperature range 30–800 °C and frequency range 1 kHz–1 MHz. With Nb-doping, the T_c of the ferroelectrics reduces and peak permittivity increases. Doping also introduces small relaxor behavior in the ferroelectrics. The dc conductivity of the ceramics decreases with doping. The remnant polarization (P_r) of the intergrowth ferroelectrics is increased with Nb doping.     

Fe2O3掺杂对氧化锌线性电阻的影响

利用固相烧结法制备出基础配方为ZnO–A1₂O3–MgO–TiO₂–SiO₂–Fe2O3的ZnO线性电阻。研究了Fe₂O₃掺杂量对ZnO线性电阻微观结构、阻温特性和阻频特性的影响。结果表明:当Fe₂O₃掺杂量为0.75%(质量分数)时,氧化锌线性电阻的非线性系数为1.1₂,阻温系数取得–8.23×10^–3/℃,此时样品的综合性能最好。