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。     

Sr(Ce_(0.6)Zr_(0.4))_(1-x)Y_xO_3质子电解质的合成研究

采用Pechini法合成了Sr(Ce_(0.6)Zr_(0.4))_(1-x)Y_xO_3(SCZY,x=0.10, 0.15, 0.20)电解质粉体,将所制粉体模压成型后在1450℃煅烧10 h得到固体电解质。采用XRD研究掺杂量和煅烧温度对粉体相纯度的影响,通过SEM观察粉体和电解质的微观结构,用电化学阻抗谱法测量电解质的电性能。结果表明:1000℃煅烧后的SCZY粉体(x=0.15)为纯的钙钛矿相,粉体晶粒尺寸随煅烧温度升高而明显长大。高速球磨能有效改善粉体的团聚情况,得到亚微米粉体,由此压制的质子电解质更加致密,没有微孔等缺陷, 800℃的电导率为7.94×10~(-3) S·cm~(-1)。     

新钽酸盐Ba2LnTi2Ta3O15(Ln=Y、La)的结构与介电性能

通过固相反应法合成了四方钨青铜结构新钽酸盐Ba2LaTi2Ta3O15与Ba2YTi2Ta3O15,分别进行了X射线衍射分析与介电性能测试.结果表明, Ba2LaTi2Ta3O15室温时晶胞参数为a=1.242 64(5) nm, c=0.391 57(2) nm,为四方钨青铜结构顺电相；Ba2YTi2Ta3O15室温时晶胞参数为a=1.236 46(4) nm, c=0.388 60(2) nm,为四方钨青铜结构铁电相,铁电相与顺电相转变温度为180 ℃.频率为1 MHz时, Ba2LaTi2Ta3O15陶瓷的室温相对介电常数为194,介电损耗也降低至8×10－4. Ba2YTi2Ta3O15陶瓷的室温相对介电常数为107.     

新铌酸盐Ba5LnZnNb9O30(Ln=Y,La)的合成、结构与介电性能

在BaO-Ln2O3-ZnO-Nb2O5(Ln=Y,La)体系中通过固相反应法合成了填满型钨青铜结构的新铌酸盐Ba5YZnNb9O30与Ba5LaZnNb9O30.采用X射线衍射分析和扫描电镜进行了结构分析,并进行了介电性能测试.结果表明,Ba5YZnNb9O30为弛豫性铁电体,10kHz时的居里温度为25℃;室温时为四方钨青铜结构铁电相,晶胞参数a=1.25255(4)nm,c=0.39530(2)nm;1MHz时陶瓷体的室温相对介电常数为456.Ba5YZnNb9O30在室温下为四方钨青铜结构顺电相,晶胞参数a=1.25731(3)nm,c=0.39812(2)nm;频率为1MHz时,其陶瓷的室温相对介电常数为316.     

Ba_(1-x)Ca_xZr_(0.2)Ti_(0.8)O_3陶瓷的微观结构、相变与介电性质（英文）

采用传统的水热合成法和烧结过程制备了Ba_(1-x)Ca_xZr_(0.2)Ti_(0.8)O_3(BCZT,x=0.1,0.2,0.3)陶瓷.研究了Ca~(2+)含量对其相组成、微观结构和介电性质所产生的影响.结果表明当x=0.3时,出现了不纯相.随着Ca~(2+)含量的增加,BCZT陶瓷的形貌从平板状转化为不规则的立方体状.介电常数曲线显示为大而宽的峰,其峰值出现在约66℃.从介电损耗曲线可以观察到随着烧结温度的增加,出现了斜方相至四方相(T_(O-T))和四方相至立方相(T_(T-C))的多晶相变.     

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.     

铁电陶瓷Pb1-xLaxTiO3的热膨胀性

通过溶胶-凝胶的方法合成了Pbl-xLaxTiO3铁电陶瓷,用X射线测定其固溶范围为0.0≤x<0.4;晶胞参数随x连续变化,呈非线性关系;当x在固溶范围内增加变化时,Pbl-xLaxTiO3由四方相向立方相转变,转变点在x=0.25附近.当x超过固溶极限xx=.4时,有少量的La2Ti2O7焦绿石相生成.通过高温X射线衍射测定了Pbl-xLaxTiO3(x=0.10、0.15、0.20、0.30)的晶胞参数随温度变化的关系,得到了本征热膨胀性;同时也提供了一种测量铁电材料居里温度的有效方法.DSC分析表明,固溶化合物Pbl-xLaxTiO3的热稳定性随着固溶度x的增加而降低.     

新铌酸盐Sr5LnTi3Nb7O30的结构与介电性能

在SrO-Ln2O3-TiO2-Nb2O5(Ln=La, Y)体系中,通过固相反应法，合成了填满型钨青铜结构新铌酸盐Sr5LaTi3Nb7O30与Sr5YTi3Nb7O30.分别采用X射线衍射分析、扫描电镜进行了结构分析,并进行了介电性能测试.结果表明, Sr5LaTi3Nb7O30室温时为四方钨青铜结构顺电相,晶胞参数a=1.233 60(4) nm, c=0.388 01(2) nm;频率为1 MHz时,其陶瓷的室温相对介电常数为466,介电损耗约为5×10－3.Sr5YTi3Nb7O30为弛豫性铁电体, 10 kHz时居里温度为260 ℃;室温时为四方钨青铜结构铁电相,晶胞参数a=1.228 80(4) nm, c=0.387 05(2) nm; 1 MHz时,陶瓷体的室温相对介电常数为290.     

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.     

ZrO2添加对BaO-La2O3-TiO2介质陶瓷介电性能的影响

BaO-La2O3-TiO2(BLT)是典型的高介电常数微波介质陶瓷,其作为微波谐振器与滤波器的关键材料,在微波通讯技术上有着重要的应用. 选用ZrO2对BLT进行改性研究,当ZrO2的加入量z＜0.5mol时,烧结体的主晶相为Ba6-3xLa8 2x(Ti1-zZrz)18O54(x=1/2)钨青铜结构(TB)固溶体,随ZrO2加入量的增多,烧结体中产生第二相,当z＝1.0mol时,烧结体的主晶相为La2Zr2O7和BaZrO3,这与结构许容因子的变化密切相关,获得较优介电性能如下εr=103.71,Q·f=4862.53 GHz,τf=168.97×10-6/℃,优于不添加ZrO2时烧结体介电性能(εr=139.73,Q·f=1238.96 GHz,τf=179.97×10-6/℃) ,说明少量ZrO2的加入可以改善BLT陶瓷的品质因数和频率温度系数,略降低介电常数. SEM分析表明,少量ZrO2的加入没有改变烧结体的微观形貌,改性前后烧结体内部均为典型的柱状TB固溶体形貌.     

Correlation of crystal structure, dielectric properties and lattice vibration spectra of (Ba(1-x)Sr(x))(Zn(1/3)Nb(2/3))O3 solid solutions

(Ba(1-x)Sr(x))(Zn(1/3)Nb(2/3))O(3) (BSZN) (x = 0.0, 0.50, 0.60, 0.65, 0.70, 1.0) solid solutions were synthesized by a conventional solid-state sintering technique. Vibration spectra (Raman spectroscopy and Fourier transform far-infrared reflection spectroscopy, FTIR) and X-ray diffraction (XRD) were employed to evaluate the crystal structures and phonon modes of these solid solutions. Dielectric constants (ε(r)) and temperature coefficient of capacitances (τ(c)) were examined to reveal the correlation of the dielectric properties and the crystal structures. The results show that with the increase in Sr(2+) content, the lattice structures of ceramics turn gradually from disordered cubic structure to ordered structure because antiphase tilting of the oxygen octahedra occurs where x≥ 0.65, which is the main reason for the phase transitions and variation of crystal structure. The appearance of the phase transitions is associated with variation of the symmetry structure, from cubic (Pm ?3m, where x = 0) to pseudocubic (I4/mcm, where 0.65 ≤x < 1.0) and then to hexagonal (P ?3ml, where x = 1.0). New phonon modes appear at around 250 cm(-1) in Raman spectra where x≥ 0.65, and there is also a different phonon mode appearing at 156 cm(-1) in the FTIR spectra at the same x range. The appearance of the new phonon modes is the characteristic of ceramics whose oxygen octahedra have tilted with Sr(2+) concentration where x≥ 0.65. The Raman shifts are related to the rigidity of the oxygen octahedra, while the widths of peaks are correlated with τ(c). The FTIR spectra were subjected to the Kramers-Kronig analysis, and the imaginary part of the dielectric constant was analyzed in detail.     

Phase evolution, phase transition, raman spectra, infrared spectra, and microwave dielectric properties of low temperature firing (K(0.5x)Bi(1-0.5x))(Mo(x)V(1-x))O4 ceramics with scheelite related structure

In the present work, the (K(0.5x)Bi(1-0.5x))(Mo(x)V(1-x))O(4) ceramics (0≤x ≤ 1.00) were prepared via the solid state reaction method and sintered at temperatures below 830 °C. At room temperature, the BiVO(4) scheelite monoclinic solid solution was formed in ceramic samples with x < 0.10. When x lies between 0.1-0.19, a BiVO(4) scheelite tetragonal phase was formed. The phase transition from scheelite monoclinic to scheelite tetragonal phase is a continuous, second order ferroelastic transition. High temperature X-ray diffraction results showed that this phase transition can also be induced at high temperatures about 62 °C for x = 0.09 sample, and has a monoclinic phase at room temperature. Two scheelite tetragonal phases, one being a BiVO(4) type and the other phase is a (K,Bi)(1/2)MoO(4) type, coexist in the compositional range 0.19 < x < 0.82. A pure (K,Bi)(1/2)MoO(4) tetragonal type solid solution can be obtained in the range 0.82 ≤ x ≤ 0.85. Between 0.88 ≤ x ≤ 1.0, a (K,Bi)(1/2)MoO(4) monoclinic solid solution region was observed. Excellent microwave dielectric performance with a relative dielectric permittivity around 78 and Qf value above 7800 GHz were achieved in ceramic samples near the ferroelastic phase boundary (at x = 0.09 and 0.10).     

Synthesis, structure and dielectric properties of Ba1-xSrx My Ti1-yO3 (M = Zr, Sn)

A series of Ba1-xSrxMyTi1-yO3 (M = Zr, Sn, 0≤x≤0.4, 0≤y≤0.3) solid solutions were synthesized with the soft chemical method below 100 ℃. XRD pattern and cell parameters-composition figures of the prepared powder demonstrate that they are completely miscible solid solutions based on BaTiO3. Furthermore, TEM shows that they have a shape of uniform, substantially spherical particles with an average particle size of 70 nm in diameter. The sintered ceramics of the powder doped with Sr2 and Zr4 or Sn4 have dielectric constant eight times higher and dielectric loss thirty per cent lower than those of pure BaTiO3 phase at room temperature.     

Hydrotherrnal synthesis, structure and property of nano-BaTiO3-based dielectric materials

A series of Ba1-xSrxTi1-yZryO3 (0≤x≤0.5, 0≤y≤0.4) and Ba1-xZnxTi1-ySnyO3 (0≤x≤0.3, 0≤y≤0.3) solid solutions were synthesized by Iow-temperature/Iow-pressure hydrothermal method below 170℃, 0.8 MPa. XRD pattern and cell parameters-composition figures of these prepared powders demonstrated that they are completely miscible solid solutions based on BaTiO3. Furthermore, TEM showed that they have a shape of uniform, substantially spherical particles with an average particle size of 70 nm in diameter. The sintered ceramics of those powders doped by Sr2+ and Zr4+ or Zn2+ and Sn4+ have dielectric constant twelve times higher than and dielectric loss 1/6 those of pure BaTiO3 phase at room temperature.     

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。     

Ba~1~-~xCa~xSn~yTi~1~-~yO~3纳米材料的、合成结构与性能

采用常压水相法,在100℃以下制备了一系列Ba~1~-~xCa~xSn~yTi~1~-~yO~3固溶体纳米粉末(0≤x≤0.5,0≤y≤0.3),经XRD物相分析和d-间距-组成图证明,产品为立方晶系的完全互溶取代固溶体,结果符合Vegard定律。TEM形貌观察,粒子为均匀球形,平均粒径70nm。通过制陶实验,分别测定了该系列固溶体的室温介电常数以及介电常数随温度的变化,结果发现,用软化学方法在BaTiO~3中掺入适量钙和锡,由于掺杂离子均匀进入母体晶格,引起T~c降低,室温介电常数达9800,经BaTiO~3纯相提高6倍,而介电损失却降低50%。     

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.     

类钙钛矿新铌酸盐Ba5NdTi2Nb3O18的合成、结构与介电特性

为满足现代通信技术的小型化、集成化与高可靠性的迫切要求,探索具有高介电常数、低介电损耗与低温度系数的微波介电材料引起了材料科学、化学、物理、电子等领域科学工作者的广泛关注,并已开发出复合钙钛矿结构Ba(Zn_(1/3)Ta_(2/3))O_3、钨青铜结     

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.     

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.