Bi含量对SrBi4Ti4O15铁电材料性能的影响

~~Bi含量对SrBi_4Ti_4O_(15)铁电材料性能的影响@朱骏$扬州大学物理科学与技术学院!江苏扬州,225002 @毛翔宇$扬州大学物理科学与技术学院!江苏扬州,225002 @卢网平$扬州大学物理科学与技术学院!江苏扬州,225002 @惠荣$扬州大学物理科学与技术学院!江苏扬州,225002 @陆文峰$扬州大学物理科学与技术学院!江苏扬州,225002 @陈小兵$扬州大学物理科学与技术学院!江苏扬州,225002~~~~~~~~     

Nd掺杂Bi4Ti3O12-SrBi4Ti4O15陶瓷的电性能

Nd等价取代Bi_4Ti_3O_(12)-SrBi_4Ti_4O_(15)的A位,形成SrBi_(8-x)Nd_xTi_7O_(27)(x=0.00～1.50)共生陶瓷.结果表明:Nd掺杂未改变晶体的共生结构,样品剩余极化(2P_r)在掺杂量x=0.50时取得极大值,为32.3×10~(-2) C·m~(-2),比未掺杂时增加了70%,而矫顽场则从未掺杂时的90.5×10~5 V·m~(-1)上升为103×10~5 V·m~(-1).Nd掺杂使得样品的居里温度(t_C)有所下降,x=0.50时的t_C为538℃.掺杂使得样品的压电性能明显改善,压电系数d_(33)从未掺杂时的6 pC·N~(-1)增加到x=0.50时的11 pC·N~(-1).     

Co掺杂Bi5Ti3FeO15多铁陶瓷的磁电性能

采用了传统的固相烧结工艺制备出Bi₅Fe_1-xCo _{x Ti3O15(BFCT-x,x=0.0—0.6)多铁陶瓷样品,研究了Co掺杂对Bi5FeTi3O15(BFTO)微观结构、铁电和磁性能的影响.X射线衍射谱显示样品均已形成四层铋系层状钙钛矿相,且随着掺杂量的增加发生了结构变化.拉曼光谱进一步证实掺入的Co占据了< 关键词： 固相烧结 多铁陶瓷 剩余磁化 剩余极化}     

脉冲激光沉积法制备高温压电薄膜0.20 BiInO$lt;sub$gt;3$lt;/sub$gt;-0.80PbTiO$lt;sub$gt;3$lt;/sub$gt;$lt;strong$gt;$lt;font color="#ff0000"$gt;$lt;font color="#ff0000"$gt;（已撤稿）$lt;/font$gt;$lt;/font$gt;$lt;/strong$gt;

采用脉冲激光沉积法制备了0.20BiInO₃-0.80PbTiO₃（20BI-PT）高温压电薄膜,并与0.15BiInO₃-0.85PbTiO₃（15BI-PT）样品进行了比较研究. X射线衍射谱显示,20BI-PT样品100峰出现了明显的劈裂,显示样品具有更高的四方对称性. FESEM图显示,20BI-PT样品中出现了部分111取向的三角形晶粒. 20BI-PT样品的铁电剩余极化（P_r）为～28 μC/cm²,矫顽场（E_c）为～120 kV/cm,相较15BI-PT样品,P_r略有增加,但同时E_c也有增加. 20BI-PT样品的横向压电系数（e_31,f）约为–4.7±0.6 C/m²,和15BI-PT相比几乎一样. 介电温度谱显示,20BI-PT 样品的居里温度比15BI-PT增加了约30 ℃,达590 ℃,且介电峰没有明显的频率依赖性. Rayleigh分析显示,20BI-PT样品中内在本征因素及可翻转畴对介电非线性的贡献和15BI-PT基本相同,但是外在因素的贡献没有15BI-PT的贡献大,这可能和20BI-PT样品中晶粒111相对取向率较高有关. 关键词： 薄膜 脉冲激光沉积 铁电 压电     

Cr掺杂对La0.75Ca0.25MnO3陶瓷材料磁性能的影响

采用传统的固相烧结工艺,制备了La0.75Ca0.25Mn1-xCrxO3(x=0,0.02,0.05,0.1)陶瓷样品,用X射线衍射对其微结构进行了分析,并测量了样品的铁磁性能.X射线谱显示样品为四方系晶体.ESR表明掺杂对样品朗德因子g几乎没有影响,而且样品总磁偶极矩的绝大部分是由自旋磁偶极矩贡献的.磁化曲线显示样品存在明显的自旋倾斜态,而掺杂可以削弱甚至破坏样品的自旋倾斜;样品热磁曲线表明,B位高掺杂导致样品晶格畸变从而使得样品磁化强度减小.     

Structure, ferroelectric and dielectric properties of Bi2WO6 with different bismuth content

This paper reports that the Bi 2 WO 6 ferroelectric ceramics with excess Bi 2 O 3 of 0.0, 2.0, 3.5 and 5.0 wt.% of the stoichiometric composition are prepared by the conventional solid-state reaction method. Their microstructure, ferroelectric properties, the concentration and mobility of the defects have been analysed systematically. With increasing Bi content, the remnant polarization decreases, and the broken-down voltage increases. The optimum Bi excess, 3.5, lowers the oxygen vacancy concentration, while further Bi-addition brings about more defects. The activation energies fitted from cole-cole plots are 0.97 eV, 1.07 eV, 1.18 eV, and 1.33 eV, respectively. This suggests that the mobility of the defects is weakened by Bi-addition, which may be due to the increase of the ratio of the number of Bi 2 O 2 layers to that of the perovskite blocks.     

Great enhancement in remnant polarization of SrBi4Ti4O15 thin films by A-site doping of Fe3+ ions

SrBi4-xFexTi4O15 (SBFT-x) thin films (x = 0.00, 0.05, 0.08, 0.15) have been synthesized on Pt/Ti/SiO2/Si (100) substrates by sol-gel method. This paper finds that Fe-doping does not change the crystal structure of SrBi4Ti4O15 (SBTi). The coercive filed (Ec) and remnant polarisation (Pr) increase at first, then decrease with the increase of Fe doping content. At a maximum applied field of 229 kV/cm, the 2Pr reaches a maximum value of 91.1 μC/cm2 at x = 0.05 and the corresponding Ec is 72 kV/cm. The 2Pr increases by about 260% and the Ec decreases by about 6%, respectively. Obviously, the ferroelectric property of SrBi4Ti4O15 is greatly enhanced by Fe doping. The fatigue-endurance characteristic of the SBFT-0.05 is not improved. After 1.1×109 read/write cycles at a frequency of 50 kHz, the nonvolatile polarisations (Pnv = P*-P∧) decreased about 48% of its initial value.     

基于PowderX软件的拉曼光谱数据处理

将处理 X射线衍射谱的 Powder X软件用于处理拉曼光谱数据 ,可方便地获得谱线中各个拉曼峰的位置、强度和半高宽等信息。经过平滑、去背景后 ,拉曼谱图的变化趋势与原始谱图吻合 ,谱线的信噪比及分辨率也有所提高 ,表明 Powder X软件完全可用于拉曼光谱的数据处理     

Bi_5Fe_(0.7)Ni_(0.3)Ti_3O_(15)多铁陶瓷的电磁性能

采用传统的固相烧结工艺制备出Bi5Fe0.7Ni0.3Ti3O15(BFNT)多铁陶瓷样品,研究镍离子基团的植入对材料的微观结构、磁性能和电性能的影响.X射线衍射谱显示BFNT样品的4层Aurivillius相已形成.室温下,BFNT样品具有铁磁性,其剩余磁化(2Mr)和矫顽场(2Hc)分别为0.086 A.m2.kg-1和18.5 kA.m-1.样品磁性的增强可能来源于局域的Fe—O—Ni的耦合.介电温度谱的测试结果表明:与Bi5FeTi3O15(BFTO)比较,BFNT的铁电相变温度降低,低温段的介电峰具有明显的弛豫特征,该弛豫可能与磁有关.室温下,当外加电场为24.5 MV.m-1时,样品的剩余极化(2Pr)和矫顽场(2Ec)分别为0.069 C.m-2和14.3 MV.m-1.     

The doping effects of BiFe1-xCoxO3 （x=0.0-0.8） in layered perovskite BiaTi3O12 ceramics

BisFe1-xCoxTi3O15 （x=0.0, 0.2, 0.4, 0.5, 0.6, and 0.8） multiferroic ceramics are synthesized in two steps using the solid state reaction technique. X-ray diffraction patterns show that the samples have four-layer Aurivillius phases. At room temperature （RT）, the samples each present a remarkable coexistence of ferromagnetism （FM） and ferroelectricity （FE）. The remnant polarization （2Pr） reaches its greatest value of 14 gC/cm2 at x = 0.6. Remnant magnetization （2Mr） first increases and then decreases, and the greatest 2Mr is 7.8 menu/g when x = 0.5. The magnetic properties for x = 0.4 are similar to those for x = 0.6, indicating that the magnetic properties originate mainly from the coupling between Fe3＋ and Co3＋ ions, rather than from their own magnetic moments.