|本期目录/Table of Contents|

[1]黄昌蓉,徐 军*.新型Ruddlesden-Popper相Sr3Sn2O7陶瓷铁电体[J].武汉工程大学学报,2017,39(03):239-242.[doi:10. 3969/j. issn. 1674?2869. 2017. 03. 006]
 HUANG Changrong,XU Jun*.New Ceramic Ferroelectric Sr3Sn2O7 with Ruddlesden-Popper Phase[J].Journal of Wuhan Institute of Technology,2017,39(03):239-242.[doi:10. 3969/j. issn. 1674?2869. 2017. 03. 006]
点击复制

新型Ruddlesden-Popper相Sr3Sn2O7陶瓷铁电体(/HTML)
分享到:

《武汉工程大学学报》[ISSN:1674-2869/CN:42-1779/TQ]

卷:
39
期数:
2017年03期
页码:
239-242
栏目:
材料科学与工程
出版日期:
2017-06-24

文章信息/Info

Title:
New Ceramic Ferroelectric Sr3Sn2O7 with Ruddlesden-Popper Phase
文章编号:
20170306
作者:
黄昌蓉12徐 军12*
1. 武汉工程大学材料科学与工程学院,湖北 武汉 430205;2. 等离子体化学与新材料湖北省重点实验室(武汉工程大学),湖北 武汉 430205
Author(s):
HUANG Changrong12 XU Jun12*
1. School of Materials Science and Engineering,Wuhan Institute of Technology,Wuhan 430205,China;2. Hubei Key Laboratory of Plasma Chemical and Advanced Materials(Wuhan Institute of Technology),Wuhan 430205,China
关键词:
Sr3Sn2O7铁电陶瓷居里温度介电性能
Keywords:
Sr3Sn2O7 ferroelectric ceramics Curie temperature dielectric property
分类号:
TM911.3
DOI:
10. 3969/j. issn. 1674?2869. 2017. 03. 006
文献标志码:
A
摘要:
为了寻求新的混合非常规铁电体,采用固相法合成了具有Ruddlesden-Popper结构的Sr3Sn2O7陶瓷,并研究了该材料的介电与铁电性能. 通过X射线衍射分析检测Sr3Sn2O7的相组成,采用扫描电镜与能谱分析仪分析Sr3Sn2O7陶瓷的微观形貌与元素含量,采用不同频率下的介电温谱测量和电滞回线测量对样品的介电与铁电性能进行表征. 结果显示,制备的Sr3Sn2O7陶瓷为单一正交相结构,其晶胞参数a=2.062 72 nm,b=0.572 49 nm,c=0.570 03 nm,样品在不同频率下测得的介电温谱在132 ℃存在一个明显的介电峰,同时其电滞回线显示明显的室温铁电性,居里温度约为132 ℃.
Abstract:
To seek new hybrid improper ferroelectricity,Sr3Sn2O7 ceramic with Ruddlesden-Popper phase was prepared by the conventional solid-state reaction method. The phase purity was characterized by X-ray diffraction,and the microstructure and composition were analyzed by scanning electron microscopy and energy dispersive system. The dielectric constant as the function of the temperature at different frequencies showed a dielectric peak at about 132 ℃,and the polarization-electric field measurement at room temperature showed a typical hysteresis loop. The results indicate that Sr3Sn2O7 ceramic has an orthorhombic structure with a=2.062 72 nm,b=0.572 49 nm and c=0.570 03 nm. The dielectric temperature spectra at different frequencies exhibit a dielectric peak at about 132 ℃. Meanwhile, a typical ferroelectric hysteresis loop reveals significant room temperature ferroelectricity and its Curie temperature is about 132 ℃.

参考文献/References:

[1] GARCIA V,BIBES M. Electronics: inside story of ferroelectric memories[J]. Nature,2012,483(7389): 279-281. [2] LIAO L,FAN H J,YAN B,et al. Ferroelectric transistors with nanowire channel: toward nonvolatile memory applications[J]. Acs Nano,2009,3(3): 700-706. [3] CHOI T,LEE S,CHOI Y J,et al. Switchable ferroelectric diode and photovoltaic effect in BiFeO3[J]. Science,2009, 324(5923): 63-66. [4] JAMIL A,KALKUR T S,CRAMER N. Tunable ferroelectric capacitor-based voltage-controlled oscillator[J]. IEEE Transactions on Ultrasonics,Ferroelectrics,and Frequency Control,2007,54(2): 222-226. [5] BENEDEK N A,FENNIE C J. Why are there so few perovskite ferroelectrics?[J]. The Journal of Physical Chemistry C,2013,117(26): 13339-13349. [6] FENNIE C J. Ferroelectrically induced weak ferromagnetism by design[J]. Physical Review Letters,2008,100(16): 167203-1-167203-4. [7] CURTAROLO S,HART G L W,NARDELLI M B,et al. The high-throughput highway to computational materials design[J]. Nature Materials,2013,12(3): 191-201. [8] BENEDEK N A,FENNIE C J. Hybrid improper ferroelectricity: a mechanism for controllable polarization-magnetization coupling[J]. Physical Review Letters,2011,106(10): 107204-1-107204-4. [9] HARRIS A B. Symmetry analysis for the Ruddlesden-Popper systems Ca3Mn2O7 and Ca3Ti2O7[J]. Physical Review B,2011,84(6): 49-51. [10] OH Y S,LUO X,HUANG F T,et al. Experimental demonstration of hybrid improper ferroelectricity and the presence of abundant charged walls in (Ca,Sr)3Ti2O7 crystals[J]. Nature Materials,2015,14(4): 407-413. [11] LIU X Q,WU J W,SHI X X,et al. Hybrid improper ferroelectricity in Ruddlesden-Popper Ca3(Ti,Mn)2O7 ceramics[J]. Applied Physics Letters,2015,106(20): 202903-1-202903-4. [12] RUDDLESDEN S N,POPPER P. New compounds of the K2NiF4 type[J]. Acta Crystallographica,1957,10(8): 538-539. [13] GREEN M A,PRASSIDES K,DAY P,et al. Structure of the n=2 and n=∞ member of the Ruddlesden-Popper series,Srn+1SnnO3n+1[J]. International Journal of Inorganic Materials,2000,2(1):35-41. [14] BOUSQUET E,DAWBER M,STUCKI N,et al. Improper ferroelectricity in perovskite oxide artificial superlattices[J]. Nature,2008,452(7188): 732-736. [15] MULDER A T,BENEDEK N A,RONDINELLI J M,et al. Turning ABO3,antiferroelectrics into ferroelectrics: design rules for practical rotation-driven ferroelectricity in double perovskites and A3B2O7,ruddlesden-popper compounds[J]. Advanced Functional Materials,2013,23(38):4810-4820. [16] LEI B F,MAN S Q,LIU Y L,et al. Luminescence properties of Sm3+- doped Sr3Sn2O7 phosphor[J]. Materials Chemistry & Physics,2010,124(Suppl. 2/3):912-915. [17] 曲远方. 功能陶瓷材料[M]. 北京:化学工业出版社,2003: 28-66. [18] SCOTT J F,DAWBER M. Oxygen-vacancy ordering as a fatigue mechanism in perovskite ferroelectrics[J]. Applied Physics Letters,2000,76(25): 3801-3803. [19] CHEN A,ZHI Y,CROSS L E. Oxygen-vacancy-related low-frequency dielectric relaxation and electrical conduction in Bi:SrTiO3[J]. Physical Review B,2000,62(1):228-236. [20] WARREN W L,VANHEUSDEN K,DIMOS D,et al. Oxygen vacancy motion in perovskite oxides[J]. Journal of the American Ceramic Society,1996,79(2):536-538.

相似文献/References:

[1]骆建国,朱 蒙,龙春艳,等.Sr1-x(YK)0.25xBa0.5xBi4Ti4O15陶瓷的制备及其介电性研究[J].武汉工程大学学报,2018,40(03):288.[doi:10. 3969/j. issn. 1674?2869. 2018. 03. 011]
 LUO Jianguo,ZHU Meng,LONG Chunyan,et al.Preparation and Dielectric Properties of Sr1-x(YK)0.25xBa0.5xBi4Ti4O15 Ceramics[J].Journal of Wuhan Institute of Technology,2018,40(03):288.[doi:10. 3969/j. issn. 1674?2869. 2018. 03. 011]

备注/Memo

备注/Memo:
收稿日期:2016-12-20作者简介:黄昌蓉,硕士研究生. E-mail:1216241042@qq.com
更新日期/Last Update: 2017-06-22