弛豫铁电铌镁酸铅的朗道系数及其临界行为的研究
[Abstract]:Relaxor ferroelectric single crystals usually have higher piezoelectric properties than traditional piezoelectric materials, which provides a broad application prospect for their applications in health detection of civil engineering structures. Although most scholars believe that the local nano-polarization region is the main reason for its high performance, the internal mechanism has not been fully recognized. In addition, due to the lack of corresponding Landau coefficient, the corresponding thermodynamic theoretical calculation can not be carried out. Combined with the phenomenon observed by experiment, the thermodynamic coefficient of Landau is obtained, and the theoretical prediction and calculation are carried out with the experimental results, and then the internal mechanism of giant piezoelectric in relaxor ferroelectric single crystal and its response in external field are deeply studied. This is of great significance for the development of a new generation of piezoelectric single crystals, especially lead-free piezoelectric single crystals. For this purpose, the following studies have been carried out in this paper: (1) the role of polar nanoparticles in relaxor is analyzed, and the state and properties of polar nanoparticles at different temperatures are determined. Considering its essential characteristics and its role in relaxor ferroelectrics, the contribution of nano-microregions to the giant piezoelectric effect is inferred by determining the phase structure properties of relaxor ferroelectrics. According to the composition-temperature phase diagram of lead magnesium niobate, the phase structure of the crystal can be classified into trihedral phase, monoclinic phase and tetrahedral phase. Combined with the phase structure and dynamic behavior under different temperature and electric field, combined with the characteristic properties of Landau's phenomenological theory, the Landau coefficient is obtained. A series of concrete test and verification methods for obtaining Landau coefficient are put forward. (2) for PMN-0.30PT single crystal with left component of quasi-homomorphism phase boundary, the double electric hysteretic line is fitted. The Landau coefficient is obtained by fitting the trend of dielectric coefficient with temperature and the temperature of tripartite and tetrahedral phase transition. Based on the obtained Landau coefficient, the ferroelectric properties are calculated by thermodynamic theory and compared with the experimental results. The energy distribution of thermodynamics and various regular statistical results are used to analyze the coexistence phase of the experiment. By determining the content of the stable phase, the performance of the coexistence region is calculated. Furthermore, the results are compared with the experimental results. (3) because the theoretical coefficients of ferroelectric Landau are mainly determined by some characteristics of single domain structure, it is necessary to ensure that the single crystal is in a single domain state after polarization. The microdomain structure can be observed by polarizing microscope. By cutting the crystal into different shapes and applying electric fields in different directions to the crystal, combined with the optical characteristics of the crystal, the change of crystal domain structure near the phase transition temperature is observed in detail. The critical electric field of the crystal under the condition of forming a single domain is analyzed and summarized. Based on the effect of electric field on domain structure, different domain structures are obtained by polarizing single crystal samples at different temperatures and electric fields. (4) for PMN-0.36PT single crystals, which are mainly tetrahedral phase at room temperature, the hysteretic loop is fitted. The dielectric coefficient and the critical electric field needed to induce the tripartite phase are obtained to obtain Landau parameters. The ferroelectric properties varying with temperature are calculated theoretically by using the obtained Landau parameters, and the results are compared with the experimental results. In addition, the multi-domain structure phase diagram of PMN-0.30PT and PMN-0.36PT thin films is derived by thermodynamic theory for the first time, and the difference and reason of phase diagram are analyzed.
【学位授予单位】:哈尔滨工业大学
【学位级别】:硕士
【学位授予年份】:2017
【分类号】:O738
【相似文献】
相关期刊论文 前10条
1 于玉兰;;冰的静态介电系数的理论计算[J];曲阜师院学报(自然科学版);1985年04期
2 王评初;殷之文;;在直流偏压作用下钽酸锂、铌酸锶钡和铌酸钡钠单晶的介电系数[J];无机材料学报;1981年Z1期
3 孔力,,徐恕宏,皮振邦,赵维毅;磁场对水介电系数作用的研究[J];华中理工大学学报;1996年05期
4 朱小娟;魏楠;张方辉;;温度对绝缘纸介电系数和损耗角正切的影响[J];陕西科技大学学报(自然科学版);2009年03期
5 赵家瑜;液晶介电系数的半电压测量法[J];华东化工学院学报;1989年01期
6 张兴元,陈王丽华,蔡忠龙;陶瓷型铁电复合物厚片介电系数的电场依赖性[J];复合材料学报;2000年03期
7 王春云;超耐热性低介电系数的聚酰亚胺绝缘膜[J];化工新型材料;1996年02期
8 崔庆谷,孙明义,江汉保,郑时龙,尤庆祥;微波场中化学试剂复介电系数及其温度特性[J];化学研究与应用;1999年01期
9 张季爽;;芳香醚浸渍剂的探讨[J];绝缘材料通讯;1981年02期
10 叶君永;杨晓庆;;等效介电系数经验公式在微波加热计算中的应用[J];化工学报;2006年10期
相关会议论文 前10条
1 华伟;杨晓庆;黄卡玛;赵岩岩;;有机二元体系等效复介电系数的实验研究[A];2005'全国微波毫米波会议论文集(第二册)[C];2006年
2 江汉保;郝晋;;不同浓度生理盐水复介电系数的微波扫频测定[A];1989年全国微波会议论文集(上)[C];1989年
3 江汉保;孙明义;华伟;吴光国;段恒清;杨友远;;无损测定成品带线基片的复介电系数[A];1993年全国微波会议论文集(下册)[C];1993年
4 包永芳;吕英华;杨显清;;负介电系数集成材料电磁特性分析——周期性单元结构对电磁特性的影响[A];第17届全国电磁兼容学术会议论文集[C];2007年
5 罗平生;王亦春;王晓莉;徐华;;基于虚拟仪器的新型电滞回线测试系统开发[A];第十七届全国测控计量仪器仪表学术年会(MCMI'2007)论文集(下册)[C];2007年
6 倪尔瑚;;用频率调谐的TE_(01)模微波谐振腔测量复介电系数[A];1985年全国微波会议论文集[C];1985年
7 王乐;罗平生;王晓莉;;电滞回线测量系统的设计与开发[A];2008’“先进集成技术”院士论坛暨第二届仪表、自动化与先进集成技术大会论文集[C];2008年
8 王恩信;候正则;姜斌;恽正中;;低烧结温度、低介电系数基极材料的研究[A];第二届中国功能材料及其应用学术会议论文集[C];1995年
9 刘显强;韩晓东;张泽;季凌飞;蒋毅坚;;激光法合成高介电系数陶瓷Ta_2O_5-TiO_2的TEM研究[A];2004年材料科学与工程新进展[C];2004年
10 刘显强;韩晓东;张泽;季凌飞;蒋亦坚;;激光法合成高介电系数陶瓷Ta2O5-TiO2晶体点阵结构的TEM/HREM研究[A];2004年中国材料研讨会论文摘要集[C];2004年
相关博士学位论文 前6条
1 华伟;复杂电磁媒质介电系数测量方法及实验研究[D];四川大学;2006年
2 杨晓庆;微波与化学反应体系相互作用过程中的特殊效应研究[D];四川大学;2006年
3 胡轶;基于声弛豫吸收谱线峰值点的气体传感技术研究[D];华中科技大学;2016年
4 董超;等离子体中温度弛豫的理论研究[D];中国科学技术大学;2014年
5 陈小明;铁电电容的性能测试方法和建模方法研究[D];复旦大学;2005年
6 王军军;四方相铌酸钠基无铅压电单晶的电学性能及电畴结构[D];哈尔滨工业大学;2016年
相关硕士学位论文 前10条
1 张杭波;弛豫铁电铌镁酸铅的朗道系数及其临界行为的研究[D];哈尔滨工业大学;2017年
2 邓腾飞;CaCu_3Ti_4O_(12)陶瓷巨介电响应及掺杂研究[D];华南理工大学;2016年
3 汪雷;低介电系数的多孔性氧化硅/CE复合材料的研究[D];西北工业大学;2015年
4 刘乃源;自极化铁酸铋薄膜电滞回线和极化稳定性研究[D];吉林大学;2015年
5 贾云浩;等离子体火焰介电系数分析及电容层析成像测量研究[D];北京交通大学;2015年
6 王思琪;四方相钙钛矿铁电超晶格压电效应机理研究[D];哈尔滨工业大学;2017年
7 卜欠欠;PT基弛豫铁电晶体生长与熔体状态的研究[D];西安工业大学;2015年
8 钱俊;新型弛豫铁电单晶PZN-PT微畴动力学研究[D];上海应用技术学院;2015年
9 孙小军;A(Fe_(0.5)Nb_(0.5))O_3(A=Ca、Sr、Ba)型巨介电材料的弛豫特性及改性研究[D];桂林理工大学;2016年
10 王梦;刚性分子混合体系中二级弛豫动力学研究[D];燕山大学;2016年
本文编号:2496045
本文链接:https://www.wllwen.com/kejilunwen/huaxue/2496045.html