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1.
测量了使用溶胶 凝胶工艺制备的 (Bi0 5Na0 5) 1 -xBaxTiO3(x =0 0 0 ,0 0 4 ,0 0 6 ,0 0 8,0 12 )系陶瓷的介电、压电、铁电和热释电性能 .由于使用了溶胶 凝胶工艺制备的粉料 ,因此所有样品的压电性能都得到了较大提高 .其中(Bi0 5Na0 5) 0 94 Ba0 0 6 TiO3系陶瓷具有该系列最大的压电常数 ,d33=173× 10 - 1 2 C N ,与传统工艺相比 ,d33提高了近4 0 % .同时 ,在一定范围内 ,随Ba含量的增加 ,材料的剩余极化Pr 和矫顽场Ec 逐渐减小 ,退极化温度逐渐降低 .对于 (Bi0 5Na0 5) 0 94 Ba0 0 6 TiO3系陶瓷 ,剩余极化和矫顽场分别为 2 5 μC cm2 和 2 8kV cm ,退极化温度约为 80℃ .  相似文献   

2.
溶胶-凝胶法制备Bi0.5Na0.5TiO3陶瓷及其电学特性   总被引:25,自引:0,他引:25       下载免费PDF全文
用溶胶-凝胶工艺成功制备出Bi05Na05TiO3纳米微粉,并利用此微粉烧结出高致密度的Bi05Na05TiO3陶瓷.这种新工艺制备的Bi05Na05TiO3陶瓷,其压电性能远远高于普通方法制备的陶瓷,其中压电常数d33和机电耦合系数kt分别高达102×10-12C/N和58%.同时发现,对于这种Bi05Na05TiO3陶瓷,室温时只需施加100kV/cm左右的交变电场,就可得到矩形度极好的饱和回线,得到的剩余极化Pr和矫顽场Ec分别为32μC/cm2和61kV/cm.而在100℃以上只需施加35kV/cm的极化电场就可使样品充分极化.  相似文献   

3.
Na1/2 Bi1/2 TiO3体系的电子结构与极化特性   总被引:1,自引:0,他引:1  
采用自洽场离散变分Xa计算方法,研究了ABO3型钙钛矿结构无铅压电陶瓷Na1/2Bi1/2TiO3体系的电子结构,分析了A,B位元素取代对Na1/2Bi1/2TiO3压电陶瓷极化性能的影响.结果表明:NBT体系压电陶瓷材料存在自发极化,B位离子位移使铁电性增强,Ba,Sr与Mn离子A,B位复合取代可降低矫顽场、提高自发极化强度,从而提高材料的铁电性能,并通过实验对此结论进行了验证.  相似文献   

4.
溶胶凝胶法制备了Na0.5Bi0.5Ti1-xMnxO3(x=0,0.02,0.04)陶瓷样品,X射线衍射(XRD)分析表明陶瓷样品均形成了单一的钙钛矿(ABO3)型结构且没有杂质相的形成.随着Mn含量的增加,XRD峰向高角度方向移动,表明Mn离子进入Na0.5Bi0.5TiO3晶格.掺杂样品均表现出室温铁磁性和铁电性.磁测量表明样品中存在复杂的磁相互作用,包括铁磁,反铁磁和顺磁相互作用.以上结果表明,通过Mn的掺杂可以使铁电材料Na0.5Bi0.5TiO3转变为多铁材料.  相似文献   

5.
采用氧化物固相反应法制备了锰掺杂改性的Ba(Zr0.06Ti0.94)O3陶瓷.研究了锰的掺杂量对Ba(Zr0.06Ti0.94)MnxO3 (BZTM)陶瓷的结构、介电和压电性能的影响.实验发现,当锰含量x<0.5 mol%时进入晶格,使材料压电性能提高,损耗减小,表现出受主掺杂的特性;当锰含量x>0.5 mo 关键词: Ba(Zr 3 陶瓷')" href="#">Ti)O3 陶瓷 锰掺杂 介电性能 压电性能  相似文献   

6.
研究了铋层化合物Sr1+xBi4-xTi4-xTaxO15(x=0—1)陶瓷的介电和铁电特性.研究发现随着x值的增大,材料的居里点由540℃降到30℃左右,但材料始终具有铁电性.对于SrBi4Ti4O15陶瓷施加120kVcm的电场仍无法得到饱和的回线,此时的剩余极化和矫顽场分别约为7μCcm2和73kVcm.对于x=04—05的材料由于它们同时具有较高的居里温度300℃—360℃,较大的剩余极化7—8μCcm2和较小的矫顽场37—47kVcm,因此是一类性能较为优良的铁电材料. 关键词: 居里温度 剩余极化 矫顽场  相似文献   

7.
张艳  王增梅  陈云飞  郭新立  孙伟  袁国亮  殷江  刘治国 《物理学报》2013,62(6):66802-066802
具有准同型相界组分的0.5Ba(Ti0.8Zr0.2)O3-0.5(Ba0.7Ca0.3)TiO3 (BZT-0.5BCT)陶瓷, 表现出优异的铁电、压电性能, 作为一种具有潜在应用前景的无铅压电材料得到广泛关注. 本文采用溶胶-凝胶方法在Si(100)基底上制备了BZT-0.5BCT压电薄膜. 使用原子力显微镜和扫描电子显微镜测量得到样品的形貌图, 形貌图表明该方法制备的无铅压电薄膜表面光滑, 晶粒大小均匀、呈半球形, 直径为80–100 nm, 厚度为1.7 μm, 膜的内部有气孔.摩擦力实验表明, 压电薄膜样品与硅针尖之间存在静电力的作用, 导致其摩擦力远大于硅针尖与SiO2之间的摩擦力, 但是两者的摩擦系数基本相同.划痕实验表明, BZT-0.5BC薄膜具有很强的法向承载能力, 但是切向抗磨损能力差, 样品的平均弹性模量为23.64 GPa± 5 GPa, 其硬度为2.7–4 GPa, 两者均略低于压电陶瓷Pb(Zr, Ti)O3材料的体态值. 关键词: BZT-BCT薄膜 纳米摩擦力 纳米压痕 纳米划痕  相似文献   

8.
研究了非化学计量和掺杂对无铅压电陶瓷 (Na1 2 Bi1 2 ) 0 .92 Ba0 .0 8TiO3的压电性能及去极化温度的影响 .研究发现A位非化学计量可以提高陶瓷的压电性能 ;B位掺杂对材料电学性能的影响规律类似于Pb(Ti,Zr)O3系压电陶瓷的相关规律 ;由于非化学计量和掺杂会影响到A位离子对B位离子与氧离子形成的BO6 八面体的耦合作用 ,影响到畴的稳定性 ,从而影响到 (Na1 2 Bi1 2 ) 0 .92 Ba0 .0 8TiO3陶瓷的去极化温度 ;所研究的陶瓷样品的去极化温度越低 ,压电系数越高 .  相似文献   

9.
采用溶胶凝胶工艺在p-Si衬底上制备了SrBi2Ta2O9/Bi4Ti3O12复合铁电薄膜. 研究了SrBi2Ta2O9/Bi4Ti3O12复合薄膜的微观结构与生长行为、铁电性能和疲劳特性. 研究表明: Si衬底Bi4Ti3O12薄膜易于沿c轴择优生长,并有利于SrBi2Ta2O9/Bi4Ti3O12复合薄膜的生长.合理的SrBi2Ta2O9/Bi4Ti3O12厚度配比能获得较好的铁电性能和优良的抗疲劳特性,SrBi2Ta2O9/Bi4Ti3O12厚度配比为1∶3的复合薄膜的剩余极化强度和矫顽电场分别为8.1 μC/cm2 和 130 kV/cm,其无疲劳极化开关次数达1011以上.  相似文献   

10.
采用溶胶-凝胶法,在氧气氛中和层层晶化的工艺条件下,成功地制备了沉积在Pt/Ti/SiO2/Si(100)衬底上的铁电性能优良的Sr2Bi4Ti5O18(SBTi)薄膜,并研究了SBTi薄膜的微结构、表面形貌、铁电性能和疲劳特性.研究表明:薄膜具有单一的层状钙钛矿结构,且为随机取向;薄膜表面光滑,无裂纹,厚度约为725nm;铁电性能测试显示较饱和、方形的电滞回线,当外电场强度为275kV/cm时,其剩余极化2Pr和矫顽场2Ec分别为24.0μC/cm2和137.8kV/cm;疲劳测试发现薄膜经过4.4×1010次极化反转后,基本没有显示疲劳.  相似文献   

11.
采用氧化固相法制备了(1-x)(Bi0.5Na0.5)TiO3-xBa(Ti0.95Zr0.05)O3(BNT-BZT)陶瓷,其中掺入量x的值分别为0,0.04,0.05,0.06,0.07.研究了BNT-BZT体系陶瓷的准同型相界以及陶瓷材料的微观结构和性能之间的关系,并探讨了陶瓷的介电性能和铁电等性能.通过探究Ba(Ti,Zr)O3(BZT)掺杂量对BNT 各性能的影响得出了当掺杂量x=0.05得到结构较为致密,介电,铁电性能较好的样本,对工业化研究和生产有重要的意义  相似文献   

12.
Applied Physics A - Mn-doped 0.948Na0.5Bi0.5TiO3–0.052BaTiO3 (NBBT94.8/5.2) lead-free single crystal with excellent piezoelectric and electromechanical coupling properties was successfully...  相似文献   

13.
Using an ordinary ceramic fabrication technique, we fabricated lead-free (1-x)(K0.5Na0.5)NbO3-xBa(Ti0.95Zr0.05)O3 ceramics with CuO sintering aid . Ba(Ti0.95Zr0.05)O3 diffuses into (K0.5Na0.5)NbO3 to form a new solid solution. The ceramics with perovskite structure possess orthorhombic phase at x≤0.04 and become tetragonal phase at x≥0.06. Both the paraelectric cubic–ferroelectric tetragonal and the ferroelectric tetragonal–ferroelectric orthorhombic phase transition temperatures decrease with increasing the concentration of Ba(Ti0.95Zr0.05)O3. The doping of CuO effectively promotes the densification of the ceramics. The coexistence of the orthorhombic and tetragonal phases at 0.04<x<0.06 and the improvement in sintering performances of the ceramics significantly enhance the piezoelectric and dielectric properties at room temperature. The ceramics with x=0.04–0.06 and y=0.75–1.50 possess excellent properties: d33=119–185 pC/N, kP=37–44%, kt=35–49%, ε=341–1129, cosδ=0.7–4.4% and Tc=312–346 °C. PACS 77.65.-j; 77.84.Dy; 77.84.-s  相似文献   

14.
Lead-free [(1?x)(Na0.5Bi0.5)?xBa]Zr1?yTiyO3 ceramics (x = 0.06, 0.085, 0.09, 0.1 and y = 0.97) have been prepared by solid-state hot-pressing sintering process. The obtained samples reveal perovskite structure. Structural, thermal expansion, heat capacity, ferroelectric and dielectric measurements have been carried out on these samples in a wide temperature range. The broad anomalies were observed in thermal expansion and heat capacity, which approximately correspond to a structural, ferroelectric and dielectric properties anomaly. These anomalies can be related to temperature features of polar regions and a formation of long-range-order ferroelectric phase. The determined Burns temperature was found to increase with increasing Ba content. The obtained results are discussed in terms of local electric and strain fields caused by a difference in the ionic radii of (Na,Bi) and Ba, and Ti and Zr ions. The NBT–BTZ system is expected to be a new promising candidate for lead-free electronic ceramics.  相似文献   

15.
In the present work, lead-free piezoelectric ceramics (Na0.5Bi0.5)TiO3xCuO–yNiO (for x = 0.0, 0.02, 0.04 and 0.06) have been prepared by a conventional solid-state reaction method. An investigation of CuO and NiO doping in bismuth sodium titanate (BNT) and a study of the structure, morphology, and dielectric and ferroelectric properties of the NBT–CuNi system have been conducted. Phase and microstructural analysis of the (Na0.5Bi0.5)TiO3 (NBT) based ceramics has been carried out using X-ray diffraction and scanning electron microscopy (SEM) techniques. Field emission scanning electron microscopy (FE-SEM) images showed that inhibition of grain growth takes place with increasing Cu and Ni concentration. The results indicate that the co-doping of NiO and CuO is effective in improving the dielectric and ferroelectric properties of NBT ceramics. Temperature-dependent dielectric studies have also been carried out at room temperature to 400 °C at different frequencies. The NBT ceramics co-doped with x = 0.06 and y = 0.06 exhibited an excellent dielectric constant ?r = 1514. The study suggests that there is enormous scope of application of such materials in the future for actuators, ultrasonic transducers and high-frequency piezoelectric devices.  相似文献   

16.
The introduction of porosity into ferroelectric ceramics has been of great interest in recent years. In particular, studies of porous lead-zirconate-titanate ceramic (PZT) have been made. In the research reported, samples of Ferroperm Pz27 with porosities of 20, 25 and 30% were studied. Very complete measurements were made of all of the physical properties relevant for ferroelectric applications including thermal conductivity and diffusivity, heat capacity, dielectric, pyroelectric, piezoelectric and elastic properties. Scanning electron micrographs indicated a change from 3-0 to 3-3 connectivity with increasing porosity. Although most of the physical properties are degraded by the presence of porosity, both piezoelectric and pyroelectric figures-of-merit are improved because of the markedly reduced relative permittivity. Porous ferroelectric ceramics are very promising materials for a number of applications.  相似文献   

17.
Lead-free (1?x)[K0.5Na0.5NbO3]?x[LiSbO3] (x=0, 0.04, 0.05 and 0.06)/(KNN-LS) ceramics were prepared by conventional solid-state reaction route (CSSR). For dense morphology pure KNN ceramic was sintered at 1120 °C and LS modified KNN ceramics were sintered at 1080 °C for 4 h, respectively. The structural study at room temperature (RT) revealed the transformation of pure orthorhombic to tetragonal structure with the increase in LS content in KNN-LS ceramics. Temperature dependent dielectric study confirmed the increase of diffuse phase transition nature with the increase in LS content in KNN-LS ceramics. The presence of orthorhombic to tetragonal (TO?T) polymorphic phase transition temperature (PPT) ~43 °C confirmed the presence of two ferroelectric (orthorhombic and tetragonal) phases in 0.95KNN-0.05LS ceramics at RT. 0.95KNN-0.05LS ceramics showed better ferroelectric and piezoelectric properties i.e., remnant polarization (Pr)~18.7 μC/cm2, coercive field (Ec)~11.8 kV/cm, piezoelectric coefficient (d33)~215 pC/N, coupling coefficient (kp)~0.415 and remnant strain ~0.07% were obtained.  相似文献   

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