(K0.52Na0.44Li0.04)(Nb0.86Ta0.10Sb0.04)O3-BiFeO3无铅压电陶瓷的电性能

采用固相法制备(1-x)(K0.52Na0.44Li0.04)(Nb0.86Ta0.10Sb0.04)O3-xBiFeO3[(1-x)LF4-xBF]无铅压电陶瓷,研究BF含量(0≤x≤0.010 00)对LF4陶瓷微观结构和电性能的影响.结果表明:所有样品均具有纯的四方钙钛矿结构,引入BF能明显改善LF4陶瓷的致密性...     

K0.5Na0.5NbO3-BaCu0.5W0.5O3无铅压电陶瓷的结构与性能

以传统固相法工艺制备(1-x)K0.5Na0.5NbO3-xBaCu0.5W0.5O3[(1-x)KNN-xBCW]无铅压电陶瓷,研究不同BCW掺量(x=0％,0.1％,0.25％,0.5％,1.0％,摩尔分数,下同)对KNN陶瓷的晶体结构和电性能的影响,结果表明:x＜0.5％时,KNN陶瓷的相结构没有改变,仍为正交相...     

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。     

Na0.5Bi0.5TiO3-Ba0.5Sr0.5Nb2O6无铅压电陶瓷的研究

采用固相法制备了(1-x)(Na0.5Bi0.5)TiO3-xBa0.5Sr0.5Nb2O6(0≤x≤1.0％)(简称(1-x)NBT-xBSN)无铅压电陶瓷,研究了不同BSN含量(x=0,0.1％,0.3％,0.5％,0.7％,1.0％,摩尔分数)样品的物相组成、显微结构及电性能.结果表明:所有样品均为纯钙钛矿结构,随掺杂量x的增加,陶瓷的相对密度pr、压电常数d33和机电耦合系数kp均先增大后降低,机械品质因子Qm和退极化温度Td则逐渐下降.该体系陶瓷具有弥散相变特征,弥散指数介于1.6～1.7.当x=0.5％时,陶瓷获得最佳性能:d33=92pC/N,kp=0.164,Qm=89,εr=650,tanδ=5.47％,pr=96.5％.     

LiBiO2掺杂对0.94(Na0.8K0.16Li0.04)0.5 Bi0.5TiO3-0.06Ba(Zr0.055Ti0.945)O3压电陶瓷性能的影响

本文采用固相反应法制备了一系列LiBiO2掺杂0.94(Na0.8K0.16Li0.04)0.5Bi0.5TiO3 -0.06BaTiO3压电陶瓷,并采用SEM、XRD等分析方法对所得产物的结构和电性能进行分析.SEM观测表明:随LiBiO2掺杂量的增加,晶粒尺寸增加.XRD分析显示,LiBiO2掺杂会导致Na2O相析出.铁电测试表明随着LiBiO2掺杂量的增加,剩余极化强度和矫顽场单调下降,样品从铁电相向反铁电相转变.压电测试结果显示:随着LiBiO2掺杂量增加,d33单调下降.与单独Li、Bi掺杂提高电性能相反,LiBiO2掺杂对提高电性能无益.     

(Ba0.85Ca0.15)(Ti0.90Zr0.06Sn0.04)O3-Fe2O3无铅压电陶瓷的性能研究

采用固相法制备了(Ba0.85Ca0.15) (Ti0.90Zr0.06Sn0.04)O3-xmol％Fe2O3(简写为BCTZS-xFe)无铅压电陶瓷.研究了不同掺杂量对该陶瓷的显微结构、介电、铁电及压电性能的影响.结果表明,所有样品均具有单一的钙钛矿结构,少量掺杂能使晶粒长大,提高电性能.在x=0.025时,具有最佳的综合电性能,压电常数d33 =515 pC/N,机电耦合系数kp=48.2％,机械品质因数Qm =182,2Pr=18.2 μC/cm2,2Ec =4.3 kV/cm,介电常数εr=5175.     

掺杂Bi_2O_3对CaCu_3Ti_4O_(12)陶瓷显微结构和介电性能的影响

采用传统高温共固相反应法制备了Ca(1-x)BixCu3Ti4O(12-x/2)(x=0,1%,2%,3%,4%,5%)陶瓷,研究了掺杂Bi2O3对CaCu3Ti4O12陶瓷的显微结构和介电性能的影响,结果表明:掺杂Bi2O3可以促进CCTO陶瓷的致密性和晶粒均匀性,掺杂Bi2O3有利于提高CCTO陶瓷的介电性能以及其稳定性,且介电性能与陶瓷晶粒的均匀性和陶瓷的致密性有着一定的联系。相对而言掺杂4%Bi2O3的介电性能最优。     

Y2O3掺杂对(Bi0.5Na0.5)0.94Ba0.06TiO3无铅压电陶瓷性能的影响研究

采用传统固相反应法制备了Y2O3掺杂(Bi0.5Na0.5)0.94Ba0.06TiO3(简写为BNBT6)陶瓷[简称为BNBT6-x(wt%)Y2O3陶瓷].研究了Y2O3 (0.2wt%～0.8wt%)掺杂对BNBT6陶瓷的结构、介电、压电、铁电性能的影响.结果表明,所有Y2O3掺杂陶瓷样品均形成了单一的钙钛矿结构;陶瓷的介电、压电、铁电性能受Y2O3掺杂的影响较为显著:当掺杂0.4wt%Y2O3时,10 kHz频率下测得的室温εr达到1530,且tanδ较小,为0.050,d33达到152 pC/N,kp=0.27,Qm=134.掺杂0.2wt%的Y2O3时BNBT6陶瓷的d33为145 pC/N,kp增大到0.29,Qm达到173,tanδ为0.053;掺杂适量Y2O3的BNBT6陶瓷铁电性能也得到改善.     

(1-x)Na0.5Bi4.5Ti4O15-xBaTiO3高温铋层状陶瓷的结构与性能研究

采用固相法制备(1-x) N0.5Bi4.5Ti4O15-xBaTiO3 (NBT-BT,x=0,0.05,0.10,0.20,0.30,0.40)高温铋层状压电陶瓷材料.用X射线衍射(XRD)、SEM扫描电镜(SEM),介电和阻抗温谱等测试方法研究了BaTiO3掺杂量对Na0.5Bi4.5Ti4O15陶瓷晶体结构和电...     

Y掺杂Ca_(1-x)Y_(2x/3)Cu_3Ti_4O_(12)陶瓷的制备及其介电性能研究

采用固相反应法制备了Y掺杂的CaCu_3Ti_4O_(12)(CCTO)陶瓷,研究了Y掺杂量对Ca_(1-x)Y_(2x/3)Cu_3Ti_4O_(12)(x=O%,1%,3%,5%)陶瓷的物相结构、微观形貌和介电性能影响,对Y掺杂影响CCTO陶瓷介电性能的机理进行了分析。结果表明:Y掺杂量在1~5 mol%时对CCTO陶瓷的相结构基本无影响;然而,当Y掺杂量达到3 mol%时,CCTO陶瓷的晶粒长大被明显抑制。Y掺杂量为1~3 mol%时,不仅可以提高CCTO陶瓷的介电常数,而且可以同步降低其介电损耗,从而有助于CCTO陶瓷的综合介电性能的提升。     

Enhanced thermal conductivity and flexural strength of sintered reaction-bonded silicon nitride with addition of (Y0.96Eu0.04)2O3

Sintered reaction-bonded silicon nitride (SRBSN) with high thermal conductivity was obtained using (Y_0.96Eu_0.04)₂O₃ and MgO as sintering additives. Green compacts were nitrided at 1400°C for 4 h. Post-sintering was carried out at 1850 and 1900°C for 4 h, respectively. In reaction-bonded silicon nitride (RBSN) doped with Y₂O₃ and MgO, the β-Si₃N₄ content and nitridation degree were 51.1% and 93.8%, respectively. However, the β-Si₃N₄ content and nitridation degree were 72.6% and 96.7% in a nitrided compact doped with (Y_0.96Eu_0.04)₂O₃ and MgO. After post-sintering, the phase composition, microstructure, mechanical properties, and thermal conductivity were investigated. After sintering at 1900°C for 4 h, the thermal conductivity of SRBSN doped with (Y_0.96Eu_0.04)₂O₃ and MgO was increased by 16.5% compared to that of the samples doped with Y₂O₃ and MgO. The highest hardness of 1639 HV and the good flexural strength of 776.4 MPa were also achieved in the sample doped with 2-mol.% (Y_0.96Eu_0.04)₂O₃ and 5-mol.% MgO.     

Broadband electromagnetic wave absorption of Ni0.5Zn0.5Nd0.04Fe1.96O4 ferrites modified by nano-silver particles

Ferrite materials have the potential to become excellent absorbing materials due to their high magnetic loss and good impedance matching. However, the disadvantages of high density and lack of dielectric loss capability limit its application. Herein, we used the citric acid sol-gel method and the self-propagating combustion method to prepare neodymium-doped nickel-zinc ferrite (NZNF), then the target effect of Sn²⁺ and an improved electroless silver plating process was used to plate a layer composed of silver nanoparticles (Ag NPs) with strong dielectric loss on the NZNF, and a magnetic/dielectric composite material (NZNF@Ag) with a heterogeneous structure was prepared. The number and particle size of Ag NPs on the surface of NZNF can be precisely controlled, thereby greatly enhancing the dielectric loss capability with little impact on the magnetic loss. The huge difference in conductivity between conductors and semiconductors promotes the occurrence of polarization at the heterogeneous interface and significantly enhances the electromagnetic wave absorption ability of the composite material. In the 2–18 GHz frequency band, the best sample can obtain an effective bandwidth of 6.82 GHz when the matching thickness is 2.1 mm. Combining conductors with semiconductor materials to obtain significantly enhanced interfacial polarization provides a new idea for improving the performance of wave absorbing materials.     

Characterization of multiferroic PbFe0.5Nb0.5O3 and PbFe0.5Ta0.5O3 ceramics derived from citrate polymeric precursors

Ceramics of the perovskite multiferroics PbFe_0.5Nb_0.5O₃ (PFN) and PbFe_0.5Ta_0.5O₃ (PFT) were synthesized from new citrate polymeric precursors. X-ray tests pointed to trace amounts of the pyrochlore phase. SEM studies revealed the heterogeneous grain size distribution for PFN and the homogeneous one for PFT. Dielectric studies pointed to one diffuse T-C phase transition at 378 K for PFN and two diffuse M-T and T-C phase transitions, at 200 and 235 K, for PFT, respectively. X-ray photoelectron spectroscopy studies of PFN reveal that all ions exist in one valence state, however, with two chemical shifts for Pb²⁺. Two valence states for the majority of ions of PFT seem to be connected with a higher volume fraction of the amorphous grain-boundary phase. The electronic energy band gap for both compounds is approximately 2.8 eV. Two magnetic transitions, ie, from the paramagnetic to the antiferromagnetic phase and then to the spin-glass phase, were observed at 156 and 10 K for PFN, and at 145 and 15 K for PFT, respectively.     

Enhanced dielectric characteristics of Ba0.94Bi0.04(Fe0.5Nb0.5)O3 coated with SiO2 and SiO2/Al2O3 over a broad frequency and temperature range

Pure phase of Ba_0.94Bi_0.04(Fe_0.5Nb_0.5)O₃ (BBFN) nano-particles were obtained by chemical co-precipitation method. The core-shell structure of BBFN@SiO₂ and BBFN@SiO₂/Al₂O₃ particles and the target ceramics were successfully prepared by aqueous chemical coating approach. The microstructures and dielectric properties of BBFN@SiO₂ and BBFN@SiO₂/Al₂O₃ were studied. Both the BBFN@SiO₂ and BBFN@SiO₂/Al₂O₃ samples show significantly decreased dielectric loss and good frequency and temperature stability on relative permittivity. Compared to the rapid decline of relative permittivity of BBFN@SiO₂, the synergistic effect of SiO₂ and Al₂O₃ in BBFN@SiO₂/Al₂O₃ ceramics made the relative permittivity of which remains a relatively high level with very low dielectric loss, making it more suitable in colossal permittivity applications. Based on the impedance analysis, the grain boundary effect and IBLC models play the important role for the improvement of dielectric properties of BBFN@SiO₂/Al₂O₃ samples.     

Phase transition behavior and electrical properties of (1 − x)Bi0.5Na0.5TiO3–x(Na0.53K0.44Li0.04)(Nb0.88Sb0.08Ta0.04)O3 lead-free ceramics

(1 ? x)Bi_0.5Na_0.5TiO₃–x(Na_0.53K_0.44Li_0.04)(Nb_0.88Sb_0.08Ta_0.04)O₃ (BNT–xNKLNST) with x = 0–0.10 lead-free piezoelectric ceramics were prepared by a solid state method, and the structure and electrical properties were investigated in this study. It is found that a morphotropic phase boundary (MPB) of rhombohedral (R) and tetragonal (T) phase exists in the range of 0.03 ≤ x ≤ 0.05 and the structure changes to paraelectric phase when x > 0.07. The samples with x = 0.05 exhibit improved electrical properties owing to the formation of MPB, which are as follows: piezoelectric constant d₃₃ = 120 pC/N, remnant polarization P_r = 39.4 μC/cm² and coercive field E_c = 3.6 kV/mm. These results indicate that the enhanced piezoelectric properties for BNT can be achieved by forming the coexistence of R and T phase.     

GdFe_(0.5)Mn_(0.5)O_3的水热合成及磁电性能的研究

采用温和的水热方法合成了GdFe0.5Mn0.5O3多铁材料,通过XRD谱图分析该化合物的结晶度非常好。磁性研究发现在25 K左右出现了顺磁-反铁磁的转变,并且在4 K和300 K时都具有磁滞回线,说明该化合物室温具有铁磁性。铁电数据显示其自发极化和电滞回线在高于居里温度附近仍然存在,这也进一步证明了此材料具有良好的室温铁电性。为此合成的该化合物GdFe0.5Mn0.5O3是一个非常有研究价值和应用前景的多铁材料。     

Sr掺杂强化LaCo0.5Cu0.5O3型钙钛矿活化过一硫酸盐的性能

采用溶胶-凝胶法制备A位掺Sr的La_xSr_1-xCo_0.5Cu_0.5O₃钙钛矿增强传统B位掺杂钙钛矿活化过一硫酸盐（PMS）的能力。本文选取效果最好的La_0.7Sr_0.3Co_0.5Cu_0.5O₃型钙钛矿为研究对象，以偶氮染料AO7为目标污染物，考察了钙钛矿投加量、PMS浓度、pH和染料废水中常见Cl^-对La_0.7Sr_0.3Co_0.5Cu_0.5O₃/PMS体系降解AO7的影响，并测试了材料的重复利用性和矿化能力。结果表明，La_0.7Sr_0.3Co_0.5Cu_0.5O₃/PMS降解AO7的速度随着材料投加量和PMS浓度的增加而加快，在中性条件下反应速度最快且矿化率良好。该体系主要活性物种之一为·OH，但Sr掺杂后钙钛矿的O空位增多使得¹O₂也参与到降解过程之中。