纳米晶钛酸钡的介电性能

采用硬脂酸凝胶法制备了纳米晶BaTiO3,用差热热重分析、红外光谱分析、X射线衍射分析等手段对产物的形成过程、晶型、粒径进行了分析.通过对材料介电性能的研究发现,纳米材料的静态介电常数远大于常规材料的介电常数,随着粒径的减小,纳米材料的介电常数先增大而后有所降低.随着环境湿度的升高,纳米晶材料的介电常数逐渐增大,在高湿度条件下,其介电常数与湿度成线性关系.     

锶、铈和镧共掺杂铈钛酸锶钡陶瓷的固溶性和介电性能的研究

采用冷压陶瓷技术,制备了(Ba1-x-0.02SrxLa0.02)(Ti1-yCey)O3(x=0.05,0.10,0.15;y=0.03,0.04,0.05)(BSLTC)陶瓷,通过X射线衍射(XRD)和介电温谱测试对BSLTC陶瓷的固溶性和介电性能进行调查。XRD结果表明,所有样品均为立方钙钛矿结构,La掺杂量为2%时,能够将(Sr,Ce)组合的固溶提高到(x=0.10,y=0.04)或(x=0.15,y=0.03)。介电结果表明,各样品的居里温度都在室温附近,介电峰明显宽化。其中,(x=0.05,y=0.03)组合的样品显示出最高的室温介电常数(ε’RT≈6000)和低介电损耗(tanδ<0.02),满足美国EIA"Y5V"高介电陶瓷材料指标。     

不同Ti/Ba比钛酸钡纳米粉体及其陶瓷的制备和介电性能研究

采用溶胶-凝胶(Sol-gel)法制备了不同Ti/Ba比的钛酸钡纳米粉体及其陶瓷。通过XRD、SEM和TEM对钛酸钡粉体及陶瓷进行了表征,并测试了陶瓷的介电性能,研究了Ti/Ba比对陶瓷微观结构和介电性能的影响。结果表明:通过溶胶-凝胶工艺制备的纳米粉体主要为立方相钛酸钡,平均粒径约19~33 nm:随Ti/Ba比的增加,钛酸钡纳米粉体平均粒径呈先稍递减后增大的趋势,当粉体平均粒径大于30 nm吋,四方相在混合相中所占比例逐渐增大;Ti/Ba=1.01~1.03时,陶瓷中异常长大的晶粒较多,室温介电常数降低;1300℃烧结2 h的Ti/Ba=1.04的钛酸钡陶瓷具有较好的介电性能。     

聚苯乙烯—钛酸钡复合材料介电性能的研究

以聚苯乙烯与化学沉淀法钛酸钡陶瓷为基本组成，采用溶液共混，溶液聚合，表面处理后溶液聚合三种方法进行复合，发现后两种复合的钛酸钡颗粒表面发生界面变化，形成活性界面，使得溶液聚合法和表面处理后溶液聚合所得到的材料具有较低的介电损耗，在高频下能保持较高的介电系数。     

溶胶-凝胶法制备掺锰钛酸钡纳米粉体及其陶瓷

The Mn-doped barium titanate nanosized powders and ceramics were prepared via the sol-gel process. The powders and ceramics were characterized by XRD， SEM and TEM. The dielectric properties of the ceramics were also measured. The influences of calcination temperature and Mn concentration on the microstructure， dielectric properties and phase composition of BaTiO₃ nano-powders and ceramics were discussed. The results indicated that the BaTiO₃-based powders doped with 1.0mol% Mn were mainly in cubic BaTiO₃ phase， but the tetragonal phase became more evident when the calcination temperature increased. After sintering， Mn-doped ceramics were mainly composed of cubic BaTiO₃. Specially， a new phase of hexagonal crystal BaTiO₃ and BaMnO₃ existed in the ceramics doped with 5.0mol% Mn and the ceramic grains were in ‘clintheriform’. The structure of ‘clintheriform’ led to the poor densification of ceramics， reducing the dielectric constant obviously. The dielectric constants of BaTiO₃ ceramics first increased and then decreased as the Mn concentration increased. The room temperature dielectric constant was 2 290 and the lowest dielectric loss was 0.004 when the Mn concentration was 0.5mol%.     

钕掺杂对（Ba0.6Sr0．4）TiO3／MgO陶瓷结构和性能的影响

采用X射线衍射、扫描电镜及介电性能测试,研究了Nd掺杂对42%(Ba0.6Sr0.4)TiO3/58%MgO(质量分数)复相陶瓷微结构和低频介电性能的影响.结果表明,添加O%～0.6%Nd203的材料均由(Ba,Sr)TiO3和Mgo两相组成,不含其他物相.随着Nd2O3掺杂量的增加,材料的晶粒尺寸变大,晶粒结合更加紧密.适量的Nd2O3掺杂可以获得适中的介电常数和较高的介电可调度,并使材料的介电损耗显著改善.0.4%(质量分数)的Nd2O3掺杂使材料的居里温度从-24.6℃迅速降低至-79.2℃,并改善了材料的温度稳定性.这时材料具有很好的介电性能,室温下(约25℃),100 kHz时介电常数为103.0,介电损耗为0.0005,2V·μm-1偏置电场下样品的介电可调度为9.15%(10 kHz),能够满足移相器的应用要求.     

CaTiO3:Zn溶胶-凝胶法制备、结构及介电性能

采用溶胶-凝胶法制备了CaTiO3:Zn纳米粒子,透射电镜图显示平均粒径为25 nm.Zn的掺杂位置对于陶瓷相组成和烧结特性有很大影响.Ca1-xZnxTiO3和CaTiO3+zZnO样品的Zn以Zn2TiO4相形式存在;而CaZnyTi1-yO3-δy=0.01)样品中的Zn进入Ti位形成固溶体,无明显的降温效果,当Zn量增至0.05和0.1时,出现ZnO相.ZnO和Zn2TiO4第二相的存在均能明显促进陶瓷烧结.CaTiO3:Zn超细粉体可在较低温度下致密烧结(≤1 250 ℃).1 250℃烧结的CaZnyTi1-yO3-δ(y=0.01)陶瓷具有较好的介电性能:介电常数ε=157,品质因数Q×f=6 819 GHz,谐振频率温度系数(τ)f=7.51×10-4℃-1.     

溶胶凝胶法制备Nd2O3改性钛酸钡陶瓷的研究

The technological condition for the preparation of BaTiO₃ ceramics doped with Nd₂O₃ by Sol-Gel was deter-mined through orthogonal experiment. When n_Ba(Ac)2∶n_Ti(OC4H9)4∶n_Nd2O3∶n_{CH3(CH2)2CH2OH}∶n_H2O=1.00∶1.00∶0.003∶7.30∶37.04, pH=3.5,T=25℃,the light-yellow-transparent-stable solution and thorough transparent gel was generat-ed, the transforming time of solution to gel was 25h. The crystal structure and particle size of BaTiO₃ ceramics doped with Nd₂O₃ were studied by SEM and X-ray respectively, the type of the crystal was tetragonal, the particle size was about 24.7nm. The dielectric constant (ε) and dielectric loss (tanδ) of BaTiO₃ ceramics doped with Nd₂O₃ were determined between 10⁴～10⁶Hz, and the results showed that the dielectric constant was increased obviously, the dielectric loss was decreased clear and the resistivity (ρ_V) was also decreased noticeably.     

CaTiO3∶Zn溶胶-凝胶法制备、结构及介电性能

采用溶胶-凝胶法制备了CaTiO3∶Zn纳米粒子,透射电镜图显示平均粒径为25 nm。Zn的掺杂位置对于陶瓷相组成和烧结特性有很大影响。Ca1-xZnxTiO3和CaTiO3+zZnO样品的Zn以Zn2TiO4相形式存在;而CaZnyTi1-yO3-δ(y=0.01)样品中的Zn进入Ti位形成固溶体,无明显的降温效果,当Zn量增至0.05和0.1时,出现ZnO相。ZnO和Zn2TiO4第二相的存在均能明显促进陶瓷烧结。CaTiO3∶Zn超细粉体可在较低温度下致密烧结(≤1 250℃)。1 250℃烧结的CaZnyTi1-yO3-δ(y=0.01)陶瓷具有较好的介电性能:介电常数ε=157,品质因数Q×f=6 819 GHz,谐振频率温度系数τf=7.51×10-4℃-1。     

锰掺杂Ba0.6Sr0.4TiO3-MgTiO3复相陶瓷的制备和介电性能

以分析纯的Ba(NO3)2、Sr(NO3)2、草酸和钛酸丁酯为原料, 采用草酸盐共沉淀法制备了钛酸锶钡（Ba0.6Sr0.4TiO3, BST）纳米粉体. XRD和SEM分析结果表明, 该方法制备出立方相的Ba0.6Sr0.4TiO3粉体, 平均粒径小于100 nm, 具有较高的烧结活性. 用传统固相法制备了锰掺杂钛酸锶钡-钛酸镁(Ba0.6Sr0.4TiO3-MgTiO3, BST-MT)复相陶瓷, 系统研究了掺杂0.1%-2.0%(x, 摩尔分数, 下同)锰对钛酸锶钡-钛酸镁复相陶瓷微观形貌和介电性能的影响机理. 结果表明, 当锰的掺杂量小于1.5%时, Mn作为受主掺杂取代占据钙钛矿ABO3的B位, 因此导致居里点略微向高温偏移和相变扩散的发生, 锰的掺杂导致晶格畸变, 促进了晶粒生长, 使晶界相比例下降, 因此介电损耗随着锰掺杂量的增大而减小; 当锰的掺杂量为1.5%时, 介电损耗达到最小值, 继续增大掺杂量, 介电常数下降, 介电损耗上升.     

A位取代对(Ca0.61Nd0.26)TiO3陶瓷烧结特性和介电性能的影响

采用常规固相反应法,以(Ca0.61Nd0.26)TiO3体系为基体成分,研究了A位取代对(Ca0.61Nd0.26)TiO3陶瓷的烧结特性和介电性能的影响规律。结果表明:Zn,Mg的A位取代,促使(Ca0.61Nd0.26)TiO3陶瓷烧结温度从1350℃降至1250℃。Zn,Mg在一定范围内A位取代(Ca0.61Nd0.26)TiO3中的Ca可形成钙钛矿结构的固溶体,Zn、Mg最大固溶度(x(Zn),y(Mg))分别不超过0.1和0.15mol。当取代量超过固溶度后,分别形成Ca2Zn4Ti15O36和MgTi2O5第二相。随Zn和Mg取代量的增加,陶瓷介电常数(εr)和谐振频率温度系数(τf)减小。陶瓷品质因数(Qf)值随Zn取代量先增后减,而随Mg取代量增加,其Qf值一直增大。Zn,Mg最佳取代分别为x(Zn)=0.15和y(Mg)=0.25,在1250℃烧结2h,[(Ca0.85Zn0.15)0.61Nd0.26]TiO3的介电性能:εr=93.60,Qf=12454GHz,τf= 150.3ppm·℃-1,[(Ca0.75Mg0.25)0.61Nd0.26]TiO3的介电性能:εr=72.48,Qf=14622GHz,τf= 108ppm·℃-1。     

Preparation and Dielectric Properties of Mn-Doped Ba0.6Sr0.4TiO3-MgTiO3 Composite Ceramics

Barium strontium titanate (Ba_0.6Sr_0.4TiO₃, BST) nano-powders were prepared using Ba(NO₃)₂, Sr(NO₃)₂, oxalic acid dehydrate, and tetrabutyl titanate (Ti(OC4H9)4) as precursors by the chemical co-precipitation method. The product was characterized by thermogravimetry-differential scanning calorimetry (TG-DSC) thermal analyses, X-ray diffraction (XRD), and scanning electron microscopy (SEM). The experimental results indicated that the resulting Ba_0.6Sr_0.4TiO₃ nano-powders were homogeneous with agglomerated nature. The Ba_0.6Sr_0.4TiO₃-MgTiO₃ (BST-MT) bulk composite ceramics doped by Mn were obtained by the traditional solid phase method. The XRD patterns demonstrated that Mn-doped BST was unable to change the perovskite crystalline structure of BST materials. SEM photographs revealed that the crystalline grains became larger with increasing the content of doping Mn (<1.5% (x, molar fraction)) and then the size of grains decreased after the Mn content exceeded 1.5% in the BST ceramics, suggesting the effect of Mn doping on the morphologies of BST-MT composites. The dielectric properties of BST-MT composite ceramics doped with 0.1%-2.0% (x) Mn were investigated systematically. Two effects of Mn doping on the dielectric properties of the BST-MT composite ceramics were observed. At low Mn doping concentrations (<1.5%), Mn mainly acted as an acceptor dopant to replace Ti at the B site of ABO3 perovskite structure, leading to a diffused phase transition. It was also observed that the grain size increased drastically as the Mn content increased and thus caused the decrease of dielectric loss. At higher Mn doping concentrations (>1.5%), the grain size decreased and the suppression of permittivity and the drastic increase of the dielectric losses were observed, which indicated a “composite” mixing effect.     

Bi掺杂对La_(0.1)Sr_(0.9)TiO_3陶瓷热电性能的影响

在5%H_2+95%N_2(V/V)还原气氛中1 500℃烧结4 h制备La_(0.1)Bi_xSr_(0.9-x)TiO_3(x=0、0.05、0.075、0.1)陶瓷,并对其组成、显微结构和热电性能进行研究。结果表明:掺Bi试样的主晶相均为Sr Ti O3,当Bi掺杂量大于0.075时,样品中出现少量Bi_2O_3杂相;掺Bi试样的晶粒发育完全,形状规则,结合紧密,显示出Bi_2O_3良好的助烧效果。另外,Bi元素掺入使La_(0.1)Sr_(0.9)TiO_3陶瓷的电导率和Seebeck系数绝对值显著增加,说明Bi元素的掺入可有效提高材料的载流子浓度和载流子迁移率。其中,x=0.075时试样的功率因子最大,在400℃时为692μW·m~(-1)·K~(-2)。虽然其热导率比未掺杂Bi试样有所提高,x=0.075时试样的ZT值在500℃时仍可达0.172,比未掺杂Bi试样提高了130%。     

Bi掺杂对La0.1Sr0.9TiO3陶瓷热电性能的影响

在5% H₂+95% N₂（V/V）还原气氛中1 500℃烧结4 h制备La_0.1Bi_xSr_0.9-xTiO₃（x=0、0.05、0.075、0.1）陶瓷,并对其组成、显微结构和热电性能进行研究。结果表明：掺Bi试样的主晶相均为SrTiO₃,当Bi掺杂量大于0.075时,样品中出现少量Bi₂O₃杂相;掺Bi试样的晶粒发育完全,形状规则,结合紧密,显示出Bi₂O₃良好的助烧效果。另外,Bi元素掺入使La_0.1Sr_0.9TiO₃陶瓷的电导率和Seebeck系数绝对值显著增加,说明Bi元素的掺入可有效提高材料的载流子浓度和载流子迁移率。其中,x=0.075时试样的功率因子最大,在400℃时为692 μW·m^-1·K^-2。虽然其热导率比未掺杂Bi试样有所提高,x=0.075时试样的ZT值在500℃时仍可达0.172,比未掺杂Bi试样提高了130%。     

Cu2+离子A位取代对MgTiO3陶瓷结构及介电性能的影响

采用固相反应制备了Mg_1-xCu_x TiO₃(0.00≤x≤0.20)微波介电陶瓷,研究CuO烧结助剂对MgTiO₃陶瓷的微观结构和微波介电性能的影响。实验结果表明,CuO中的Cu²⁺离子会进入到MgTiO₃晶格中并取代Mg²⁺,形成Mg_1-xCu_x TiO₃固溶体。由于液相效应,适量的CuO可以促进MgTiO₃陶瓷的致密化烧结,降低其烧结温度。Cu²⁺离子的A位取代会改变样品的TiO₆八面体扭曲度。随着Cu²⁺离子含量的增加,会使MgTiO₃陶瓷的结构稳定性降低。随着CuO含量的增加,晶粒的不均匀生长和液相的出现导致样品的品质因数(Qf)下降。同时,Mg_1-xCu_x TiO₃陶瓷的相对密度、结构...     

Ba0.6Sr0.4TiO3/聚偏氟乙烯-聚甲基丙烯酸甲酯复合材料的制备及其介电性能

采用流延热压工艺制备Ba_0.6Sr_0.4TiO₃(BST)/聚偏氟乙烯(PVDF)?聚甲基丙烯酸甲酯(PMMA)复合薄膜,研究了PMMA含量对复合材料微观组织结构和介电性能的影响规律。结果表明,BST相能够均匀分散在聚合物基体中,归因于PMMA与PVDF良好的相容性,2种聚合物之间的界面不分明;随着PMMA含量的增加,复合材料的介电常数先降低后升高,耐击穿强度和介电可调性先增加后减少。PMMA含量(体积分数)为15%的BST/PVDF?PMMA₁₅复合材料的综合性能最佳:介电常数为23.2,介电损耗为0.07,耐击穿强度为1412 kV·cm^-1,在550 kV·cm^-1偏压场下,介电可调性为26.2%。     

掺杂Sm_2O_3的Y_2O_3-2TiO_2系微波介质陶瓷的性能研究

以具有中介电常数的新型Y2O3-2TiO2系微波介质陶瓷为基体,选用Sm2O3作为掺杂改性剂,通过传统固相法制备成陶瓷。重点研究了不同Sm2O3掺杂量对基体Y2O3-2TiO2微波介质陶瓷物相组成和介电性能的影响。采用X射线衍射和扫描电子显微镜分别对其物相组成和显微结构进行了分析,用阻抗分析仪和网络分析仪测试其介电性能。结果表明:掺杂Sm2O3未改变材料的主晶相,仍为A2B2O7烧绿石结构,Sm3+取代Y3+占据A位;掺杂有效降低了陶瓷的烧结温度,掺杂量为5%(质量分数)时,烧结温度为1330℃,材料的综合性能最佳,εr=23,tanδ=0.0046,Q×f=6713 GHz。     

Bi2O3掺杂对Ag(Nb0.8Ta0.2)O3陶瓷结构和介电性能的影响

本文研究了Bi₂O₃掺杂对Ag(Nb_0.8Ta_0.2)O₃陶瓷的结构和介电性能的影响。X射线衍射(XRD)结果表明,Bi₂O₃的掺杂可以使陶瓷中Ag⁺被还原并析出,且银析出的量随Bi₂O₃掺杂量的增加而不断增加,这可能源自于Bi³⁺对Ag⁺的取代。在一定范围内增大Bi₂O₃掺杂量可提高Ag(Nb_0.8Ta_0.2)O₃陶瓷的室温介电常数,降低介电损耗,并使温度系数向负值方向移动。当Bi₂O₃的掺杂量约为3.5wt%时,样品具有较大的介电常数(ε=672)和较小的介电损耗(tanδ=7.3×10^-4)。     

Bi_2O_3掺杂对Ag(Nb_(0.8)Ta_(0.2))O_3陶瓷结构和介电性能的影响(英文)

本文研究了Bi2O3掺杂对Ag(Nb0.8Ta0.2)O3陶瓷的结构和介电性能的影响。X射线衍射(XRD)结果表明,Bi2O3的掺杂可以使陶瓷中Ag+被还原并析出,且银析出的量随Bi2O3掺杂量的增加而不断增加,这可能源自于Bi3+对Ag+的取代。在一定范围内增大Bi2O3掺杂量可提高Ag(Nb0.8Ta0.2)O3陶瓷的室温介电常数,降低介电损耗,并使温度系数向负值方向移动。当Bi2O3的掺杂量约为3.5wt%时,样品具有较大的介电常数(ε=672)和较小的介电损耗(tanδ=7.3×10-4)。