Piezoelectric and electro—optic properties of tetragonal (1-x)Pb(Mg1/3Nb2/3)O3—xPbTiO3 single crystals by phenomenological theory

doi:10.1088/1674-1056/24/7/077701

中国物理B ›› 2015, Vol. 24 ›› Issue (7): 77701-077701.doi: 10.1088/1674-1056/24/7/077701

• CONDENSED MATTER: ELECTRONIC STRUCTURE, ELECTRICAL, MAGNETIC, AND OPTICAL PROPERTIES • 上一篇下一篇

Piezoelectric and electro—optic properties of tetragonal (1-x)Pb(Mg_1/3Nb_2/3)O₃—xPbTiO₃ single crystals by phenomenological theory

邱建华, 王秀琴, 袁宁一, 丁建宁

Center for Low-dimensional Materials, Micro-nano Devices and System, Changzhou University, Changzhou 213164, China

收稿日期:2015-01-13 修回日期:2015-02-10 出版日期:2015-07-05 发布日期:2015-07-05
基金资助:
Project supported by the National Natural Science Foundation of China (Grant No. 51335002), the Changzhou Science and Technology Project, China (Grant No. CJ20130022), and the Priority Academic Program Development of Jiangsu Higher Education Institutions, China.

Piezoelectric and electro—optic properties of tetragonal (1-x)Pb(Mg_1/3Nb_2/3)O₃—xPbTiO₃ single crystals by phenomenological theory

Qiu Jian-Hua (邱建华), Wang Xiu-Qin (王秀琴), Yuan Ning-Yi (袁宁一), Ding Jian-Ning (丁建宁)

Center for Low-dimensional Materials, Micro-nano Devices and System, Changzhou University, Changzhou 213164, China

Received:2015-01-13 Revised:2015-02-10 Online:2015-07-05 Published:2015-07-05
Contact: Qiu Jian-Hua, Ding Jian-Ning E-mail:jhqiu@cczu.edu.cn;dingjn@cczu.edu.cn
Supported by:
Project supported by the National Natural Science Foundation of China (Grant No. 51335002), the Changzhou Science and Technology Project, China (Grant No. CJ20130022), and the Priority Academic Program Development of Jiangsu Higher Education Institutions, China.

摘要/Abstract

摘要：

An eighth-order Landau–Devonshire theory is constructed to investigate the piezoelectric and electro–optic properties of tetragonal (1-x)Pb(Mg_1/3Nb_2/3)O₃–xPbTiO₃ single crystals (x=0.38 and x=0.4). The dielectric stiffness coefficients of the Landau potential are obtained by fitting to the dielectric properties and the phase transition temperature between cubic phase and tetragonal phase. It is indicated that tetragonal (1-x)Pb(Mg_1/3Nb_2/3)O₃–xPbTiO₃ single crystals have the first-order cubic-tetragonal phase transitions. The dielectric constants are in great agreement with the experimental results. The piezoelectric coefficients d₃₃ and d₃₁ at room temperature are about 145 pC/N and -62 pC/N respectively which are smaller than that of (1-x)Pb(Mg_1/3Nb_2/3)O₃–xPbTiO₃ single crystals around the morphotropic phase boundary. Moreover, tetragonal (1-x)Pb(Mg_1/3Nb_2/3)O₃–xPbTiO₃ single crystals have the linear electro–optic coefficients r_c=33.7 pm/V and r_c=28.8 pm/V for x=0.38 and x=0.4, respectively which are in accordance with the measurements.

关键词: dielectric property, piezoelectric property, electrooptic effect

Abstract:

Key words: dielectric property, piezoelectric property, electrooptic effect

中图分类号: (Dielectric properties of solids and liquids)

77.22.-d

77.65.Bn (Piezoelectric and electrostrictive constants) 78.20.Jq (Electro-optical effects)

邱建华, 王秀琴, 袁宁一, 丁建宁. Piezoelectric and electro—optic properties of tetragonal (1-x)Pb(Mg_1/3Nb_2/3)O₃—xPbTiO₃ single crystals by phenomenological theory[J]. 中国物理B, 2015, 24(7): 77701-077701.

Qiu Jian-Hua (邱建华), Wang Xiu-Qin (王秀琴), Yuan Ning-Yi (袁宁一), Ding Jian-Ning (丁建宁). Piezoelectric and electro—optic properties of tetragonal (1-x)Pb(Mg_1/3Nb_2/3)O₃—xPbTiO₃ single crystals by phenomenological theory[J]. Chin. Phys. B, 2015, 24(7): 77701-077701.

参考文献 28

[1]	Li X B and Luo H S 2010 J. Am. Ceram. Soc. 93 2915
[2]	Noheda B, Cox D E, Shirane G, Gao J and Ye Z G 2002 Phys. Rev. B 66 054104
[3]	Feng Z Y, Zhao X Y and Luo H S 2006 J. Am. Ceram. Soc. 89 3437
[4]	Fang S X, Tang D Y, Chen S M, Zhang H and Liu Y L 2015 Chin. Phys. B 24 027802
[5]	Li F, Zhang S J, Xu Z, Wei X Y, Luo J and Shrout T R 2010 J. Appl. Phys. 108 034106
[6]	He C J, Xu F, Wang J M, Du C L, Zhu K J and Liu Y W 2011 J. Appl. Phys. 110 083513
[7]	He C J, Fu X D, Xu F, Wang J W, Zhu K J, Du C L and Liu Y W 2012 Chin. Phys. B 21 054207
[8]	Park S E and Shrout T R 1997 J. Appl. Phys. 82 1804
[9]	He C J, Zhou Z X, Liu D J, Zhao X Y and Luo H S 2006 Appl. Phys. Lett. 89 261111
[10]	Wan X M, Xu H Q, He T H, Lin D and Luo H S 2003 J. Appl. Phys. 93 4766
[11]	He C J, Ge W W, Zhao X Y, Xu H Q, Luo H S and Zhou Z X 2006 J. Appl. Phys. 100 113119
[12]	Wan X M, Wang D Y, Zhao X Y, Luo H S, Chan H L W and Choy C L 2005 Solid State Commun. 134 547
[13]	Jeong D Y, Lu Y, Sharma V, Zhang Q M and Luo H S 2003 Jpn. J. Appl. Phys. 42 4387
[14]	Feng Z Y, Zhao X Y and Luo H S 2004 J. Phys.: Condens. Matter 16 6771
[15]	Noblanc O, Gaucher P and Calvarin G 1996 J. Appl. Phys. 79 4291
[16]	Li Y L, Cross L E and Chen L Q 2005 J. Appl. Phys. 98 064101
[17]	The list of the parameters of G (in SI units, the temperature T in ℃) used in the calculations. For x=0.38: T0=162.1, C=7.13×105, α11=-1.7×108, α111=6.9×109, and α1111=1.4×1010. For x=0.4: T0=175.6, C=5.95×105, α11=-1×108, α111=3.9×109, and α1111=1×1010
[18]	Emelyanov A Y, Pertsev N A and Kholkin A L 2002 Phys. Rev. B 66 214108
[19]	Di Domenico M and Wemple S H 1969 J. Appl. Phys. 40 720
[20]	Zhao X Y, Wang J, Chew K H, Chan H L W, Choy C L, Yin Z W and Luo H S 2004 Mater. Lett. 58 2053
[21]	Tang Y X, Wan X M, Zhao X Y, Pan X M, Lin D, Luo H S, Sun J L, Meng X J and Chu J H 2005 J. Appl. Phys. 98 084104
[22]	Huan M J, Furman E, Jang S J, Mckinstry H A and Cross L E 1987 J. Appl. Phys. 62 3331
[23]	Li F, Jin L, Xu Z, Wang D W and Zhang S J 2013 Appl. Phys. Lett. 102 152910
[24]	Li F, Zhang S J, Xu Z, Wei X Y and Shrout T R 2011 Adv. Funct. Mater. 21 2118
[25]	Feng Z Y, Zhao X Y and Luo H S 2006 J. Appl. Phys. 100 024104
[26]	Wan X M, Luo H S, Wang J, Chan H L W and Choy C L 2004 Solid State Commun. 129 401
[27]	Emelyanov A S, Raevskaya S I, Savenko F I, Topolov V Y, Raevski I P, Turik A V and Kholkin A L 2007 Solid State Commun. 143 188
[28]	Guo Y P, Luo H S, Ling D, Xu H Q, He T H and Yin Z W 2003 J. Phys.: Condens. Matter 15 L77

Piezoelectric and electro—optic properties of tetragonal (1-x)Pb(Mg_1/3Nb_2/3)O₃—xPbTiO₃ single crystals by phenomenological theory

Piezoelectric and electro—optic properties of tetragonal (1-x)Pb(Mg_1/3Nb_2/3)O₃—xPbTiO₃ single crystals by phenomenological theory

RichHTML

PDF (PC)

赞

可视化

摘要/Abstract

引用本文

使用本文

参考文献 28

相关文章 10

Metrics

本文评价

推荐阅读 0

[1]	Xue Wang(王雪), Shi-Xie Jiang, Lin Huang(黄林), Zi-Hui Chi(迟子惠), Dan Wu(吴丹), and Hua-Bei Jiang. Wideband frequency-dependent dielectric properties of rat tissues exposed to low-intensity focused ultrasound in the microwave frequency range[J]. 中国物理B, 2023, 32(3): 34305-034305.
[2]	徐德刚, 朱先立, 王与烨, 李吉宁, 贺奕俽, 庞子博, 程红娟, 姚建铨. Optical-induced dielectric tunability properties of DAST crystal in THz range[J]. 中国物理B, 2019, 28(12): 127701-127701.
[3]	邱建华, 陈智慧, 王秀琴, 袁宁一, 丁建宁. Dielectric and piezoelectric properties of (110) oriented Pb(Zr_1-xTi_x)O₃ thin films[J]. 中国物理B, 2016, 25(5): 57701-057701.
[4]	宋荟荟, 周万城, 罗发, 卿玉长, 陈马林. Microwave dielectric properties of Nextel-440 fiber fabrics with pyrolytic carbon coatings in the temperature range from room temperature to 700 ℃[J]. 中国物理B, 2015, 24(8): 88107-088107.
[5]	Rajwali Khan, 方明虎. Dielectric and magnetic properties of (Zn, Co) co-doped SnO₂ nanoparticles[J]. 中国物理B, 2015, 24(12): 127803-127803.
[6]	宋育全, 周卫平, 房勇, 杨艳婷, 王辽宇, 王敦辉, 都有为. Multiferroic properties in terbium orthoferrite[J]. 中国物理B, 2014, 23(7): 77505-077505.
[7]	刘荣灯, 刘蕴韬, 陈东风, 何伦华, 闫丽琴, 王志翠, 孙阳, 王芳卫. Al-doping-induced magnetocapacitance in the multiferroic CuCrS₂[J]. 中国物理B, 2013, 22(2): 27507-027507.
[8]	娄艳辉, 宋桂林, 常方高, 王照奎. Investigation on dependence of BiFeO₃ dielectric property on oxygen content[J]. 中国物理B, 2010, 19(7): 77702-077702.
[9]	龙云泽, 李蒙蒙, 隋万美, 孔庆山, 张磊. Electrical, dielectric and surface wetting properties of multi-walled carbon nanotubes/nylon-6 nanocomposites[J]. 中国物理B, 2009, 18(3): 1221-1226.
[10]	蒋青, 吴华. A possible coupling mechanism between magnetism and dielectric properties in EuTiO₃[J]. 中国物理B, 2002, 11(12): 1303-1306.