On the parameters for electrocaloric effect predicted by indirect method

doi:10.1088/1674-1056/26/11/117701

中国物理B ›› 2017, Vol. 26 ›› Issue (11): 117701-117701.doi: 10.1088/1674-1056/26/11/117701

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

On the parameters for electrocaloric effect predicted by indirect method

Hong-Bo Liu(刘宏波)

School of Materials Engineering, Shanghai University of Engineering Science, Shanghai 201620, China

收稿日期:2017-06-29 修回日期:2017-08-05 出版日期:2017-11-05 发布日期:2017-11-05
基金资助:
Project supported by the Natural Science Foundation of Shanghai, China (Grant No. 17ZR1447200).

On the parameters for electrocaloric effect predicted by indirect method

Hong-Bo Liu(刘宏波)

School of Materials Engineering, Shanghai University of Engineering Science, Shanghai 201620, China

Received:2017-06-29 Revised:2017-08-05 Online:2017-11-05 Published:2017-11-05
Contact: Hong-Bo Liu E-mail:bohongliu@gmail.com
Supported by:
Project supported by the Natural Science Foundation of Shanghai, China (Grant No. 17ZR1447200).

摘要/Abstract

摘要： The influences of specific heat capacity C_P, temperature step △T, electric field step △ E, and initial electric field E₁ on predicted electrocaloric (EC) temperature △ T of monodomain BaTiO₃ are examined by combining the Maxwell equation and phenomenological theory. Since the procedure is similar to indirect measurement of the EC effect, the results can serve as a reference for experiments. The results suggest that (i) it is reasonable to use zero-field C_P, (ii) optimized △ T should be 2 K, (iii) it is better to keep △ E<E_C, and (iv) E₁<E_C. Here, E_C is the coercive field of material.

关键词: electrocaloric effect, indirect method, BaTiO₃

Abstract: The influences of specific heat capacity C_P, temperature step △T, electric field step △ E, and initial electric field E₁ on predicted electrocaloric (EC) temperature △ T of monodomain BaTiO₃ are examined by combining the Maxwell equation and phenomenological theory. Since the procedure is similar to indirect measurement of the EC effect, the results can serve as a reference for experiments. The results suggest that (i) it is reasonable to use zero-field C_P, (ii) optimized △ T should be 2 K, (iii) it is better to keep △ E<E_C, and (iv) E₁<E_C. Here, E_C is the coercive field of material.

Key words: electrocaloric effect, indirect method, BaTiO₃

中图分类号: (Pyroelectric and electrocaloric effects)

77.70.+a

刘宏波. On the parameters for electrocaloric effect predicted by indirect method[J]. 中国物理B, 2017, 26(11): 117701-117701.

Hong-Bo Liu(刘宏波). On the parameters for electrocaloric effect predicted by indirect method[J]. Chin. Phys. B, 2017, 26(11): 117701-117701.

参考文献 31

[1]	Mischenko A, Zhang Q, Scott J, Whatmore R and Mathur N 2006 Science 311 1270
[2]	Neese B, Chu B, Lu S G, Wang Y, Furman E and Zhang Q 2008 Science 321 821
[3]	Kar-Narayan S and Mathur N D 2009 Appl. Phys. Lett. 95 242903
[4]	Epstein R I and Malloy K J 2009 J. Appl. Phys. 106 064509
[5]	Jia Y and Sungtaek Ju Y 2012 Appl. Phys. Lett. 100 242901
[6]	Gu H, Qian X, Li X, Craven B, Zhu W, Cheng A, Yao S C and Zhang Q M 2013 Appl. Phys. Lett. 102 122904
[7]	Plaznik U, Kitanovski A, Rožič B, Malič B, Uršič H, Drnovšek S, Cilenšek J, Vrabelj M, Poredoš A and Kutnjak Z 2015 Appl. Phys. Lett. 106 043903
[8]	Wang Y D, Smullin S J, Sheridan M J, Wang Q, Eldershaw C and Schwartz D E 2015 Appl. Phys. Lett. 107 134103
[9]	Blumenthal P, Molin C, Gebhardt S and Raatz A 2016 Ferroelectrics 497 1
[10]	Sette D, Asseman A, Gérard M, Strozyk H, Faye R and Defay E 2016 APL Mater. 4 091101
[11]	Liu Y, Scott J F and Dkhil B 2016 APL Mater. 4 064109
[12]	Liu Y, Scott J F and Dkhil B 2016 Appl. Phys. Rev. 3 031102
[13]	Wang X Y, Chu R J, Wei S N, Dong Z C, Zhong C G, Cao H X, Sciences S O and University N 2015 Acta Phys. Sin. 64 117701(in Chinese)
[14]	Pelaiz-Barranco A, Wang J and Yang T 2016 Ceram. Int. 42 229
[15]	Le Goupil F, Berenov A, Axelsson A K, Valant M and Alford N M 2012 J. Appl. Phys. 111 124109
[16]	Kar-Narayan S and Mathur N 2010 J. Phys. Appl. Phys. 43 032002
[17]	Kaddoussi H, Lahmar A, Gagou Y, Asbani B, Dellis J L, Cordoyiannis G, Allouche B, Khemakhem H, Kutnjak Z and El Marssi M 2016 J. Alloy. Compd. 667 198
[18]	Moya X, Stern-Taulats E, Crossley S, González-Alonso D, Kar-Narayan S, Planes A, Mañosa L and Mathur N D 2013 Adv. Mater. 25 1360
[19]	Liu H and Yang X 2015 AIP Adv. 5 117134
[20]	Akcay G, Alpay S P, Mantese J V and Rossetti G A 2007 Appl. Phys. Lett. 90 2909
[21]	Wang Y L, Tagantsev A K, Damjanovic D, Setter N, Yarmarkin V K, Sokolov A I and Lukyanchuk I A 2007 J. Appl. Phys. 101 104115
[22]	Merz W J 1953 Phys. Rev. 91 513
[23]	Pertsev N, Zembilgotov A and Tagantsev A 1998 Phys. Rev. Lett. 80 1988
[24]	Bell A and Cross L 1984 Ferroelectrics 59 197
[25]	Lines M E and Glass A M 1977(Oxford:Oxford University Press) p. 67
[26]	Ma Y B, Novak N, Koruza J, Yang T, Albe K and Xu B X 2016 Phys. Rev. B 94 100104
[27]	Ma Y B, Novak N, Albe K and Xu B X 2016 Appl. Phys. Lett. 109 242903
[28]	Novak N, Kutnjak Z and Pirc R 2013 Europhys. Lett. 103 47001
[29]	Bai Y, Ding K, Zheng G P, Shi S Q and Qiao L 2012 Phys. Status Solidi A 209 941
[30]	Bai Y, Han X, Zheng X C and Qiao L 2013 Sci. Rep. 3 2895
[31]	Qian X S, Ye H J, Zhang Y T, Gu H, Li X, Randall C and Zhang Q 2014 Adv. Funct. Mater. 24 1300

On the parameters for electrocaloric effect predicted by indirect method

On the parameters for electrocaloric effect predicted by indirect method

RichHTML

PDF (PC)

赞

可视化

摘要/Abstract

引用本文

使用本文

参考文献 31

相关文章 15

Metrics

本文评价

推荐阅读 0

[1]	刘宏波. Electrocaloric effect enhanced thermal conduction of a multilayer ceramic structure[J]. 中国物理B, 2020, 29(8): 87701-087701.
[2]	刘义, 畅艳芬, 孙阳, 沈俊, 闫丽琴, 卢遵铭. Electrocaloric effect and pyroelectric properties of organic-inorganic hybrid (C₂H₅NH₃)₂CuCl₄[J]. 中国物理B, 2019, 28(11): 117701-117701.
[3]	刘宏波. Effect of an electric field on the electrocaloric response of ferroelectrics[J]. 中国物理B, 2018, 27(12): 127701-127701.
[4]	王洪艳, 丁发柱, 古宏伟, 张腾. Strongly enhanced flux pinning in the YBa₂Cu₃O_7-X films with the co-doping of BaTiO₃ nanorod and Y₂O₃ nanoparticles at 65 K[J]. 中国物理B, 2015, 24(9): 97401-097401.
[5]	杜颜伶, 王春雷, 李吉超, 张新华, 王芙凝, 刘剑, 祝元虎, 尹娜, 梅良模. Two-dimensional metallic behavior at polar MgO/BaTiO₃ (110) interfaces[J]. , 2015, 24(3): 37301-037301.
[6]	侯志文, 康爱国, 马维清, 赵晓龙. Dimension effects on the dielectric properties of fine BaTiO₃ ceramics[J]. 中国物理B, 2014, 23(11): 117701-117701.
[7]	王洪艳, 丁发柱, 古宏伟, 张腾, 彭星煜. Precursor evolution and growth mechanism of BTO/YBCO films by TFA-MOD process[J]. 中国物理B, 2014, 23(10): 107402-107402.
[8]	丁发柱, 古宏伟, 张腾, 王洪艳, 屈飞, 邱清泉, 戴少涛, 彭星煜. Strong flux pinning enhancement in YBa₂Cu₃O_7-x films by embedded BaZrO₃ and BaTiO₃ nanoparticles[J]. 中国物理B, 2013, 22(7): 77401-077401.
[9]	邱建华, 丁建宁, 袁宁一, 王秀琴. Composition and misfit strain dependence of electrocaloric effect of Pb_1-xSr_xTiO₃ thin films[J]. 中国物理B, 2013, 22(1): 17701-017701.
[10]	邱建华, 丁建宁, 袁宁一, 王秀琴. Effect of misfit strain on the electrocaloric effect of polydomain epitaxial ferroelectric thin films[J]. 中国物理B, 2012, 21(9): 97701-097701.
[11]	彭静, 吴传菊, 孙堂友, 赵文宁, 吴小锋, 刘文, 王双保, 揭泉林, 徐智谋. Fabrication and optical properties of InGaN/GaN multiple quantum well light emitting diodes with amorphous BaTiO₃ ferroelectric film[J]. 中国物理B, 2012, 21(6): 67702-067702.
[12]	何小亢, 曾立波, 吴琼水, 张丽艳, 朱恪, 刘玉龙. Determination of elastic, piezoelectric, and dielectric constants of an R:BaTiO₃ single crystal by Brillouin scattering[J]. 中国物理B, 2012, 21(6): 67801-067801.
[13]	袁昌来, 刘心宇, 周昌荣, 许积文, 杨云. boldmath Characterization of the BaBiO₃-doped BaTiO₃ positive temperature coefficient of a resistivity ceramic using impedance spectroscopy with T_c=155℃[J]. 中国物理B, 2011, 20(4): 48701-048701.
[14]	肖长江, 迟振华, 李凤英, 冯少敏, 靳常青, 王晓慧, 邓湘云, 李龙土. Ferroelectric behaviour of 30nm BaTiO₃ ceramics prepared by high pressure assisted sintering[J]. 中国物理B, 2007, 16(10): 3125-3128.
[15]	吕国伟, 程波林, 沈　鸿, 陈玉金, 周岳亮, 陈正豪, 杨国桢. Optical properties of carbon nanotubes and BaTiO₃ composite thin films[J]. 中国物理B, 2006, 15(8): 1815-1818.