检索规则说明:AND代表“并且”;OR代表“或者”;NOT代表“不包含”;(注意必须大写,运算符两边需空一格)
检 索 范 例 :范例一: (K=图书馆学 OR K=情报学) AND A=范并思 范例二:J=计算机应用与软件 AND (U=C++ OR U=Basic) NOT M=Visual
作 者:徐泽 娄路遥 赵纯林 汤浩正 刘亦轩 李昭 齐晓梅 张波萍[2] 李敬锋 龚文 王轲 Xu Ze;Lou Lu-Yao;Zhao Chun-Lin;Tang Hao-Cheng;Liu Yi-Xuan;Li Zhao;Qi Xiao-Mei;Zhang Bo-Ping;Li Jing-Feng;Gong Wen;Wang Ke(State Key Laboratory of New Ceramics and Fine Processing,School of Materials Science and Engineering,Tsinghua University,Beijing 100084,China;School of Materials Science and Engineering,University of Science and Technology Beijing,Beijing 100083,China;Advanced Ceramic Materials&Devices Research Center,Yangtze Delta Region Institute of Tsinghua University,Zhejiang,Jiaxing 314006,China)
机构地区:[1]清华大学材料学院,新型陶瓷与精细工艺国家重点实验室,北京100084 [2]北京科技大学材料科学与工程学院,北京100083 [3]浙江清华长三角研究院,先进陶瓷材料与器件研究中心,嘉兴314006
出 处:《物理学报》2020年第12期184-192,共9页Acta Physica Sinica
基 金:国家自然科学基金优秀青年科学基金(批准号:51822206);科学挑战专题(批准号:TZ2018003);清华大学自主科研计划(批准号:20183080006)资助的课题。
摘 要:(K0.5Na0.5)NbO3基无铅压电陶瓷具有出色的综合铁电压电性能,已经初步满足了部分实际应用场景的需求.近期的研究发现,某些元素的掺杂对优化(K0.5Na0.5)NbO3基陶瓷的机电耦合性能起着至关重要的作用.本文将MnO2添加到KNbO3和(K0.5Na0.5)NbO3两种压电陶瓷中,对比研究了Mn掺杂对两种陶瓷微观结构和宏观电学性能的不同影响,分析了造成这些差异的微观物理机理.实验结果表明,掺杂后的两种陶瓷中均存在Mn2+.Mn掺杂会使KNbO3陶瓷的铁电畴尺寸减小、居里温度降低、拉曼光谱中的振动峰宽化、相变过程变得弥散,并呈现出束腰电滞回线和可回复的双极场致应变曲线;在(K0.5Na0.5)NbO3陶瓷中掺杂Mn后,其性能变化却显著不同,陶瓷的铁电畴尺寸无明显变化、居里温度未发生变化、拉曼光谱中的振动峰未发生宽化,呈现出饱和的矩形电滞回线和不可回复的双极场致应变曲线.这可能是因为,(K0.5Na0.5)NbO3陶瓷相比KNbO3陶瓷具有更大的离子无序度和晶格畸变,从而使得Mn掺杂所产生的影响相对减小.Potassium sodium niobate(K0.5Na0.5)NbO3-based lead-free piezoelectric ceramics are excellent ferroelectric materials and have been demonstrated to have many practical applications.Recent studies have revealed that chemical doping plays a crucial role in optimizing the electromechanical coupling properties of(K0.5Na0.5)NbO3-based piezoelectric ceramics.In this paper,MnO+2 is doped into potassium niobate(KNbO3)and(K0.5Na0.5)NbO3 piezoelectric ceramics prepared by the conventional solid-state reaction method.The influences of doped Mn cation on KNbO3 and(K0.5Na0.5)NbO3 piezoelectric ceramics including microstructure and macroscopic electrical properties are systematically investigated.The doping effects of Mn cation on the KNbO3 and(K0.5Na0.5)NbO3piezoelectric ceramics are significantly different from each other.For the Mn-doped KNbO3 piezoelectric ceramics,the sizes of ferroelectric domains are reduced.Meanwhile,the diffused orthorhombic-tetragonal phase transition is observed,which is accompanied by reducing dielectric loss and Curie temperature,and broadening vibration peaks in Raman spectrum.It is known that the oxygen vacancy can be formed to compensate for the charges created by the acceptor doping of Mn into the B site of perovskite,and thus forming a defect dipole with the acceptor center.From the ferroelectric measurement,a double hysteresis loop(P-E curve)and a recoverable electric-field-induced strain due to the formation of defect dipole are observed.On the contrary,for the Mn-doped(K0.5Na0.5)NbO3 piezoelectric ceramics,the sizes of ferroelectric domains are not reduced.Meanwhile,the Curie temperature and vibration peaks in Raman spectrum are not changed.A rectangular hysteresis loop(P-E curve)and an unrecoverable electric-field-induced strain are observed in the ferroelectric measurement.The difference between these systems might originate from the greater ionic disorder and lattice distortion in(K0.5Na0.5)NbO3 piezoelectric ceramics.The difference in ionic radius between Na+and K+can affect the migrati
分 类 号:TM221[一般工业技术—材料科学与工程]
正在载入数据...
正在载入数据...
正在载入数据...
正在载入数据...
正在载入数据...
正在载入数据...
正在载入数据...
正在链接到云南高校图书馆文献保障联盟下载...
云南高校图书馆联盟文献共享服务平台 版权所有©
您的IP:216.73.216.31