Dielectric properties of La2O3-doped Ba0.8Sr0.2TiO3 ceramics

La₂O₃-doped Ba_0.8Sr_0.2TiO₃ dielectric ceramics were prepared by conventional solid state ceramic route. Scanning electron microscope was employed to observe the surface morphologies. The capacitance C and dielectric loss factor D of the samples were measured with automatic LCR Meter 4225 at 10 kHz respectively. The results show that: ε _r of the samples decreases and tgδ first decreases then increases with increasing amount of La₂O₃ doping. ε _r reaches better value, tgδ obtains the minimum value at 0.5 mol% La₂O₃. ε _r increases and tgδ decreases when sintering temperature increases. The samples doped with 0.5 mol% La₂O₃ sintered at 1,350 °C for 10 h exhibited attractive properties, including high relative dielectric constant (>4,000), low dielectric loss (16.8 × 10^?4), low temperature coefficient of relative dielectric constant(<±21 %) in the temperature range of +25 to +85 °C.     

La0.8Pb0.2Fe0.8Ni0.2O3纳米粉体的制备及其CO气敏性能研究

采用柠檬酸法制备了多晶La0.8Pb0.2Fe0.8Ni0.2O3,并对其结构、电导特性和CO气敏特性进行了研究.结果表明,该材料属正交晶系钙钛矿结构,显示了p型半导体导电特性,并且在工作温度120～340℃范围内对CO气体均具有较高灵敏度,显示出对CO气体的良好气敏性能.     

阴极材料Ba0.5Sr0.5Co0.8Fe0.2O3-δ的制备和性能

用共沉淀法合成了具有单一的立方型钙钛矿结构的新型阴极材料Ba0.5Sr0.5Co0.8Fe0.2O3-δ,研究了材料的电导率和热膨胀系数与温度的关系.结果表明,前驱体在1100℃煅烧3 h后形成具有单一的立方型钙钛矿结构尺寸小于1 μm的Ba0.5Sr0.5Co0.8Fe0.2O3-δ粉末;在500～600℃致密材料的电导率高于100 S/cm,热膨胀系数随着温度的升高从13.62×10-6逐渐增大到18.75×10-6,当温度超过700℃后急剧增大.致密材料热膨胀系数在高温下剧增的主要原因是材料中比较大的氧损失.     

La3+掺杂Co0.5Ni0.5(Fe0.5Cr0.5)2O4尖晶石红外辐射材料的研究

用固相合成法制备La3+掺杂Co0.5Ni0.5(Fe0.5 Cr0.5)2O4尖晶石体系红外辐射材料,并通过DTA-TG、XRD和IRE-2型红外辐射测试等方法研究了材料的结构特征与红外辐射性能的关系,结果表明:随着La3+含量的增加,La3+以不同的形式进入Co0.5Ni0.5(Fe0.5 Cr0.5)2O4体系中,当La2O3掺杂浓度为5%(质量分数)时,样品的法向全波段辐射率达到0.91.     

尖晶石型Ni0.8Zn0.2Fe2O4纳米晶体的制备及电磁性能研究

以金属离子的柠檬酸盐为前驱体，通过sol-gel自燃烧的合成方法制备了镍锌铁氧体（Ni0．8Zn0．2Fe2O4）纳米晶体。采用FT-IR、DSC-TG、XRD、TEM波导等方法对产物以及产物的电磁性能进行了表征。结果表明，在前驱体中，金属离子与柠檬酸以络合物的形式存在，凝胶在220℃完成自燃烧反应，随着热处理温度的升高，粉体的粒径逐渐增大，纳米晶体在8-12GHz的测试条件下具有介电损耗与磁损耗，随着涂层厚度的增加，混合媒质的微波反射率逐渐增加，反射率吸收峰随着厚度的增加向低频移动。     

脉冲激光沉积Ba0.5Sr0.5TiO3、Pb0.5Ba0.5TiO3和Pb0.5Sr0.5TiO3薄膜及其介电性质

采用脉冲激光沉积法,在Pt／Ti／SiO2／Si基底上分剐制备厚度为350nm的Ba0.5Sr0.5TiO3(BST)、Pb0.5Ba0.5TiO3(PBT)和Pb0.5Sr0.5TiO3(PST)薄膜并研究了它们的介电性质。XRD显示,在相同的制备条件下三者具有不同的择优取向,PST具有(110)择优取向,PBT具有(111)择优取向,而BST则是混合取向。SEM显示三者样品表面均匀致密,颗粒尺寸大约在50nm至150nm之间。PST与BST、PBT相比有更高的介电常数,在频率为10kHz时,分别为874、334和355,而损耗都较低,分别为0．0378、0．0316和0．0423,同时PST漏电流也是最小的。测量薄膜的C-V特性扣铁电性能表明室温下BST呈现的是顺电相,PST和PBT则呈铁电相。本文也测量了薄膜在不同频率下的介电温度特性,BST、PBT和PST均表现出频率弥散现象,即随着频率的降低．居里温度降低而介电常数会升高。并测得BST和PST的居里温度分剐为-75和150℃。而PBT的居里温度在250℃以上。本文研究表明：与BST相比较,PBT的介电常数与之相近,漏电流较大;而PST具有高介电常数,较小的漏电流和较大的电容-电压调谐度,在相关半导体器件中的应用将有很大的潜力。     

Co0.8Mn0.8Ni0.9Fe0.5O4 纳米粉体的制备及热敏特性研究

采用共沉淀法,以NH4HCO3为沉淀剂制备了Co0.8Mn0.8Ni0.9Fe0.5O4负温度系数(NTC)热敏电阻纳米粉体材料,研究了不同预烧温度对材料相结构的影响,探讨了不同烧结工艺对NTC热敏电阻材料微观结构和热敏性能的影响. 采用X射线衍射(XRD)、综合热分析(TG/DTA)、红外(FT-IR)、扫描电子显微技术(SEM)和激光粒度分析仪对制备的样品进行了表征. 结果表明,750℃预烧后的粉体为纯尖晶石相,晶粒粒度为32.1nm,颗粒粒径在50～100nm范围内. 通过对不同烧结程序的对比研究发现,当烧结程序为:840℃、1200℃各保温2h,升降温速率为1℃/min时,样品电学性能较好:ρ25℃=1183Ω*cm,B25/50=3034K. 分析表明,该烧结程序能有效改善热敏电阻材料的微观结构和热敏性能. 根据ln ρ-1/T曲线斜率计算了经不同工艺烧结后热敏电阻材料的激活能在0.26eV左右.     

Influence of manganese dioxide and Ba2Co2Fe12O22‐additives on the magnetic power loss of Ni0.8Zn0.2Fe2O4 ferrites

Manganese dioxide and Ba₂Co₂Fe₁₂O₂₂ added Ni_0.8Zn_0.2Fe₂O₄ ferrites were prepared by solid state reaction process. The structure and magnetic properties of the ferrites were investigated by X‐ray diffractometer and magnetic flux density‐magnetic field analyzer. It was found that the magnetic loss shows increase‐decrease‐increase variation trend with the increase of manganese dioxide additive concentration, and the optimal concentration of manganese dioxide doping is about 1.2 wt.%. Compared with the sample without manganese dioxide doping, further investigation revealed that the hysteresis loss coefficient and eddy current loss coefficient decreased in 1.2 wt.% manganese dioxide doping nickel zinc ferrite, but the residual loss coefficient increased with manganese dioxide doping.     

Magnetic and dielectric properties of Ni0.8Zn0.2Fe2O4/HDPE composites for high-frequency application

A low loss high-frequency magnetic composite with Ni_0.8Zn_0.2Fe₂O₄ (NZO) ultrafine particles embedded in a high density polyethylene (HDPE) matrix was fabricated by using a simple low-temperature hot-pressing technique. The magnetic and dielectric properties of the as-prepared composites were investigated in details. The results indicate that as the volume of the ceramic fillers increase, the permittivity, permeability, dielectric and magnetic loss of the composite all increase. The cut-off frequencies of the composites are all above 1 GHz. Because of the low resistivity of NZO, the dielectric losses of the composites are big and decrease with frequency below 100 MHz. Good frequency stabilities of the permittivities and permeabilities, and low dielectric and magnetic losses within the measurement range have been observed. For the composite containing 30 vol% NZO, the permittivity, dielectric loss, permeability and magnetic loss are 3.7, 0.0025, 2.2 and 0.002 at 100 MHz, respectively.     

Dielectric behaviour and magnetoelectric effect in cobalt ferrite-barium titanate composites

Composites of BaTiO₃ and CoFe₂O₄ have been prepared with various compositions by double sintering method. The presence of the two phases has been confirmed by XRD. Variation of dielectric constant with temperature in these samples has been studied. All the samples have shown linear magnetoelectric conversion in the presence of static magnetic field. The magnetoelectric effect (dE/dH) has been studied as a function of intensity of magnetic field. The maximum value of the conversion factor (dH/dH)_max was found to be 0·16 mV/cm/Oe.     

LiLaPO4-coated Li[Ni0.5Co0.2Mn0.3]O2 and AlF3-coated Li[Ni0.5Co0.2Mn0.3]O2 blend composite for lithium ion batteries

A blended composite of LiLaPO₄-coated Li[Ni_0.5Co_0.2Mn_0.3]O₂ and AlF₃-coated Li[Ni_0.5Co_0.2Mn_0.3]O₂ was tested as the cathode of lithium secondary batteries. The rate capability, cyclic performance, and thermal stability of the blended electrode were characterized and compared with pristine, AlF₃-coated, and LiLaPO₄-coated electrodes. The blended sample showed good cyclic performance and thermal stability, which implies that blending these two cathode coatings were effective in obtaining their advantages and lessening their weaknesses.     

柠檬酸法和聚乙烯醇法制备La0.8Sr0.2Co0.5Fe0.5O3纳米材料工艺过程及微观形貌比较

以分析纯的硝酸镧、硝酸锶、硝酸钴和硝酸铁为原料,通过柠檬酸法(Citrate)和聚乙烯醇法(PVA)合成了LSCF纳米粉体.采用热重(TG)、差热分析(DTA)、傅立叶红外光谱(FT-IR)、X射线粉末衍射(XRD)、扫描电子显微镜(SEM)、透射电镜(TEM)和BET等技术比较研究了两种方法合成LSCF的成胶过程,晶相形成过程和微观形貌等的异同,并比较了它们的制备成本.结果表明,二种方法均在800℃煅烧可得到钙钛矿纯相,成相过程中都有碳酸锶生成.柠檬酸法和聚乙烯醇法所得粉体粒度分别30.8nm和34.2nm;比表面积分别为37.4m2/g和28.2m2相似文献   

Ba0.5Sr0.5Co0.8Fe0.2O3-δ-Ce0.9Gd0.1O2-δ中低温固体氧化物燃料电池复相阴极的研究

采用溶胶-凝胶法制备Ba_0.5Sr_0.5Co_0.8Fe_0.2O_3-δ(BSCF)粉体后, 使用Ce_0.9Gd_0.1O_2-δ(GDC)溶胶包裹BSCF粉的方法制备疏松多孔的BSCF-xGDC(x=30wt%, 40wt%, 50wt%)复相阴极。通过X射线衍射仪、场发射扫描电镜和透射电镜对复相阴极的物相组成、单电池断面形貌及GDC对BSCF颗粒的包裹形貌进行表征。利用阻抗谱测试研究了复相阴极材料的电化学性能, 讨论了掺入GDC量对阴极性能的影响。结果表明：通过GDC溶胶包裹BSCF粉体的制备方法改善了阴极的电化学性能, 在同一温度下, BSCF-40GDC阴极的极化电阻最小, 在650℃时阴极极化阻抗约为0.397 Ω•cm²; 以BSCF-40GDC为阴极制备的单电池, 以H₂+3%H₂O为燃料气、空气为氧化气体, 650℃下电池的最大功率密度为0.514 W/cm², 欧姆电阻为0.257 Ω•cm², 两极极化电阻为0.0588 Ω•cm²。     

La0.2Ba0.8(Co0.2Fe0.8)1-xZrxO3-δ透氧膜材料的微结构与氧分离性能研究

采用固相法制备了La0.2Ba0.8(Co0.2Fe0.8)1-xZrxO3-δ(x=0、0.05、0.1、0.15)片状陶瓷膜,用稳态法测试了不同成分制备样品的透氧性能,并利用XRD和SEM手段分析研究了样品的相结构和晶粒形貌及它们对材料性能的影响.研究表明固相法较难合成x=0的纯钙钛矿相,可用改进的Pechini法合成,另B位Zr的替代有利于去除材料中非钙钛矿杂相;x=0.1的样品中有少量BaZrO3析出,并导致晶粒细化(1～2μm),而这种微结构状态稳定且不受高温长时间退火和氧分压梯度的影响.晶粒细化样品的力学性能和氧渗透性能均有较大提高,x=0.1的样品较x=0样品的氧渗透性能提高了一个数量级,在1010℃,样品厚1.2mm时体系的透氧率达到4.6×10-7mol.cm-2.s-1.     

W型Ba0．8La0．2Co2Fe16O27微波吸收材料的制备与表征

采用柠檬酸溶胶凝胶法制备了稀土W型六角铁氧体Ba0.8La0.2Co2Fe16O27粉晶,用DSC-TGA、FT-IR、XRD、SEM分析了样品的形成过程、微观形貌、粒径和晶体结构,根据微波矢量网络分析仪测试的样品在2～18GHz微波频率范围的电磁参数计算了电磁损耗角正切及微波反射率.研究结果表明, 煅烧2h能得到单一的W型相Ba0.8La0.2Co2Fe16O27 ;晶粒为六角块状结构,大小均为200nm左右;Ba0.8La0.2Co2Fe16O27样品厚度为1.9mm时,12GHz位置处吸收峰为16.2dB,10dB频宽为4.0GHz;微波吸收主要由磁损耗引起.     

Dispersion characteristics of sol-gel derived (Ba0.2Pb0.8)TiO3 at various pH

The sol-gel derived (Ba_0.2Pb_0.8)TiO₃ powder was observed for suspension behaviour as a function of pH (pH 1 to 13). The dispersion has an isoelectric point (IEP) at pH 7, and better dispersion was found at lower and higher pH than at pH 7. The powder has a BET surface area of 2.3 m² g^–1 at pH 7 and 97 to 105 m² g^–1 at pH 1, 11 and 13. The sol-gel specimens derived from well dispersed suspensions with pH 11 and 13 showed a high relative density (95 to 98%).     

Nanoparticle dispersion and electroactive phase content in polyvinylidene fluoride/Ni0.5Zn0.5Fe2O4 nanocomposites for magnetoelectric applications

Ni0.5Zn0.5FeO4 ferrite/polyvinylidene fluoride composite films were prepared by a solution method and melt processing. As nanoparticle dispersion and polymer electroactive phase content are some of the key factors for improving magnetoelectric coupling in the composites, the dispersion of ferrite nanoparticles in the polymeric matrix was studied by preparing samples by two alternative dispersion routes: ultrasound and citric acid nanoparticle surfactation. The nucleation of the electroactive beta-phase of the polymer was observed in composites produced by nanoparticle dispersion by ultrasound. This fact avoids the need of stretching composites at elevated temperature in order to obtain the electroactive phase and obtain magnetoelectric composites. By this method, nevertheless, large nanoparticle agglomerates are obtained. Nanoparticle dispersion is largely improved by citric acid surfactation of the nanoparticles. On the other hand, the beta-phase of the polymer is not nucleated due to the modification of the nanoparticle-polymer interaction due to the presence of the surfactant.