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Research Article | Open Access

Composition-tailor induced electrocaloric effect near room temperature in (Pb,Ba)HfO3 films

Xian-Xiong Huanga,b,Peng-Zu GeaTian-Fu ZhangcQiu-Xiang LiuaYan-Ping JiangaZhen-Hua TangaXiao-Bin GuoaXin-Gui Tanga( )
School of Physics & Optoelectric Engineering, Guangdong University of Technology, Guangzhou, 510006, China
Jewelry Institute, Guangzhou Panyu Polytechnic, Guangzhou, 511483, China
School of Materials Science and Engineering, Harbin Institute of Technology, Shenzhen, Guangdong, 518055, China

Peer review under responsibility of The Chinese Ceramic Society.

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Graphical Abstract

Abstract

More and more researchers start to pay attention to the electrocaloric temperature change (∆T) in polar materials, which is caused by an applied electric field. In this paper, Ba-doped PbHfO3 (PBH) films were prepared by sol-gel method. Their components, microstructures, dielectric polarization and electrocaloric effects (ECEs) were investigated. With the addition of Ba2+, PBH films went from antiferroelectric (AFE) to ferroelectric (FE). At the same time, their dielectric peaks shifted toward lower temperature. The maximum ∆T obtained in Pb0.8Ba0.2HfO3 FE film is 41.1 K, which is an order of magnitude larger than PbHfO3 film (∆T ~ −4 K at 50 ℃) and Pb0.9Ba0.1HfO3 film (∆T < 4 K at 120 ℃). In order to explain this phenomenon, the Landau-Devonshire theory was adopted. Our analysis shows that the rapid variation of energy barrier height near the phase transition temperature is beneficial to obtain large polarization change and high △T, which is needed in solid-state cooling devices.

References

[1]

Wang Y, Zhang Z, Usui T, Benedict M, Hirose S, Lee J, Kalb J, Schwartz D. A high-performance solid-state electrocaloric cooling system. Science 2020;370:129-33.

[2]

Jian XD, Lu B, Li DD, Yao YB, Tao T, Liang B, Lin XW, Guo JH, Zeng YJ, Lu SG. Enhanced electrocaloric effect in Sr2+-modified lead-free BaZrxTi1-xO3 ceramics. ACS Appl Mater Interfaces 2019;11:20167-73.

[3]

Fähler S, Rößler UK, Kastner O, Eckert J, Eggeler G, Emmerich H, Entel P, Müller S, Quandt E, Albe K. Caloric effects in ferroic materials: new concepts for cooling. Adv Energy Mater 2012;14:10-9.

[4]

Liu Y, Scott JF, Dkhil B. Direct and indirect measurements on electrocaloric effect: recent developments and perspectives. Appl Phys Rev 2016;3:031102.

[5]

Zhang Y, Li W, Wang Z, Qiao Y, Xia H, Song R, Zhao Y, Fei W. Perovskite Sr1-x(Na0.5Bi0.5)xTi0.99Mn0.01O3 thin films with defect dipoles for high energy-storage and electrocaloric performance. ACS Appl Mater Interfaces 2019;11:37947-54.

[6]

Peng B, Zhang Q, Gang B, Gjt Leighton, Shaw C, Milne SJ, Zou B, Sun W, Huang H, Wang Z. Phase-transition induced giant negative electrocaloric effect in a lead-free relaxor ferroelectric thin film. Energy Environ Sci 2019;12:1708-17.

[7]

Liu Y, Dkhil B, Defay E. Spatially resolved imaging of electrocaloric effect and the resultant heat flux in multilayer capacitors. ACS Energy Lett 2016;1:521-8.

[8]

Torelló A, Lheritier P, Usui T, Nouchokgwe Y, Gérard M, Bouton O, Hirose S, Defay E. Giant temperature span in electrocaloric regenerator. Science 2020;370:125-9.

[9]

Bo Y, Zhang Q, Cui H, Wang M, Zhang C, He W, Fan X, Lv Y, Fu X, Liang J, Huang Y, Ma R, Chen Y. Electrostatic actuating double-unit electrocaloric cooling device with high efficiency. Adv Energy Mater 2021;11:2003771.

[10]

Moya X, Kar-Narayan S, Mathur ND. Caloric materials near ferroic phase transitions. Nat Mater 2014;13:439-50.

[11]

Ponomareva I, Lisenkov S. Bridging the macroscopic and atomistic descriptions of the electrocaloric effect. Phys Rev Lett 2012;108:167604.

[12]

Nair B, Usui T, Crossley S, Kurdi S, Guzmán-Verri GG, Moya X, Hirose S, Mathur ND. Large electrocaloric effects in oxide multilayer capacitors over a wide temperature range. Nature 2019;575:468-72.

[13]

Li J, Li J, Wu HH, Qin S, Su X, Wang Y, Lou X, Guo D, Su Y, Qiao L, Bai Y. Giant electrocaloric effect and ultrahigh refrigeration efficiency in antiferroelectric ceramics by morphotropic phase boundary design. ACS Appl Mater Interfaces 2020;12:45005-14.

[14]

Li J, Chang Y, Yang S, Tian Y, Hu Q, Zhuang Y, Xu Z, Li F. Lead-free bilayer thick films with giant electrocaloric effect near room temperature. ACS Appl Mater Interfaces 2019;11:23346-52.

[15]

Li JJ, Li JT, Wu HH, Qin SQ, Su XP, Wang Y, et al. Giant electrocaloric effect and ultrahigh refrigeration efficiency in antiferroelectric ceramics by morphotropic phase boundary design. ACS Appl Mater Interfaces 2020;12:45005-14.

[16]

Ge PZ, Jian XD, Lin XW, Tang XG, Zhu Z, Liu QX, Jiang YP, Zhang TF, Lu SG. Composition dependence of giant electrocaloric effect in PbxSr1-xTiO3 ceramics for energy-related applications. J. Materiomics 2019;5:118-26.

[17]

Ge PZ, Tang XG, Meng K, Huang XX, Li SF, Liu QX, Jiang YP. Energy storage density and charge-discharge properties of PbHf1-xSnxO3 antiferroelectric ceramics. Chem Eng J 2022;429:132540.

[18]

Kaur N, Chudasama B. Tunable Curie temperature of Mn0.6Zn0.4Fe2O4 nanoparticles. J Magn Magn Mater 2018;465:164-8.

[19]

Wang CL, Zhong WL, Zhang PL. The Curie temperature of ultra-thin ferroelectric films. J Phys Condens Matter 1992;3:4743-9.

[20]

Huang XX, Zhang TF, Gao RZ, Huang HB, Ge PZ, Tang H, Tang XG. Large room temperature negative electrocaloric effect in novel antiferroelectric PbHfO3 films. ACS Appl Mater Interfaces 2021;13:21331-7.

[21]

Huang XX, Zhang TF, Wang W, Ge PZ, Tang XG. Tailoring energy-storage performance in antiferroelectric PbHfO3 thin films. Mater Des 2021;204:109666.

[22]

Wilcox DL, Cook RL. Dielectric behavior in the systems PbHfO3-BaHfO3 and PbHfO3-SrHfO3. J Am Ceram Soc 1963;46:343-8.

[23]

Pokharel BP, Pandey D. Effect of Ba2+ substitution on the stability of the antiferroelectric and ferroelectric phases in (Pb1-xBax)ZrO3: phenomenological theory considerations. Phys Rev B 2002;65:214108.

[24]

Hao X, Zhai J, Yao X. A comprehensive investigation on the phase transformation behavior and electrical properties of (Pb1-xBax)ZrO3 (0 ≤ x ≤ 0.5) thin films. J Appl Phys 2008;104:124101.

[25]

Zhong WL. Phenomenological study of the size effect on phase transitions in ferroelectric particles. Phys Rev B 1994;50:698-703.

[26]

Huang H, Sun CQ, Hing P. Surface bond contraction and its effect on the nanometric sized lead zirconate titanate. J Phys Condens Matter 2000;12:L127-32.

[27]

Zhuo F, Li Q, Gao J, Ji Y, Yan Q, Zhang Y, Wu HH, Xi XQ, Chu X, Cao W. Giant negative electrocaloric effect in (Pb,La)(Zr,Sn,Ti)O3 antiferroelectrics near room temperature. ACS Appl Mater Interfaces 2018;10:11747-55.

[28]

Neese B, Chu BJ, Lu SG, Wang Y, Furman E, Zhang QM. Large electrocaloric effect in ferroelectric polymers near room temperature. Science 2008;321:821-3.

[29]

Mischenko AS, Zhang Q, Scott JF, Whatmore RW, Mathur ND. Giant electrocaloric effect in thin-film PbZr0.95Ti0.05O3. Science 2006;311:1270-1.

[30]

Sun Y, Zhang L, Wang H, Guo M, Lou X, Wang D. Composition-driven inverse-to-conventional transformation of electrocaloric effect and large energy storage density in strontium modified Ba(Zr0.1Ti0.9)O3 thin films. J Mater Chem C 2020;8:1366-73.

[31]

Shirsath SE, Cazorla C, Lu T, Zhang L, Tay YY, Lou X, Liu Y, Li S, Wang D. Interface-charge induced giant electrocaloric effect in lead free ferroelectric thin-film bilayers. Nano Lett 2020;20:1262-71.

[32]

Park MH, Kim HJ, Kim YJ, Moon T, Kim KD, Hwangn CS. Toward a multifunctional monolithic device based on pyroelectricity and the electrocaloric effect of thin antiferroelectric HfxZr1-xO2 films. Nano Energy 2015;12:31-140.

[33]

Peng B, Fan H, Zhang Q. A giant electrocaloric effect in nanoscale antiferroelectric and ferroelectric phases coexisting in a relaxor Pb0.8Ba0.2ZrO3 thin film at room temperature. Adv Funct Mater 2013;23:2987-92.

[34]

Geng W, Liu Y, Meng X, Bellaiche L, Scott JM, Dkhil B, Jiang A. Giant negative electrocaloric effect in antiferroelectric La-doped Pb(ZrTi)O3 thin films near room temperature. Adv Mater 2015;27:3165-9.

[35]

Zhang M, Liu L, Yang R, Yu P, Zhang Q, Peng B. Giant electrocaloric effect in BiFeO3 and La codoped PbZr0.7Ti0.3O3 epitaxial thin films in a broad temperature range. J. Materiomics 2022;8:156-65.

[36]

Yang J, Zhao Y, Zhu L, Hao X. Enhanced electrocaloric effect of relaxor potassium sodium niobate lead-free ceramic via multilayer structure. Scripta Mater 2021;193:97-102.

[37]

Gao R, Shi X, Wang J, Zhang G, Huang H. Designed giant room-temperature electrocaloric effects in metal-free organic perovskite [MDABCO](NH4)I3 by phase-field simulations. Adv Funct Mater 2021;31:2104393.

[38]

Wang K, Shi X, Gao R, Wang J, Xu J, Cheng X, Hunag H. Pressure-induced room temperature electrocaloric effect in BiFeO3-PbTiO3 solid solution based on landau-devonshire theory. Mater Today Commun 2022;31:103396.

[39]

Li J, Wu HH, Li J, Su X, Yin R, Qin S, Guo D, Su Y, Qiao L, Lookman T, Bai Y. Room-temperature symmetric giant positive and negative electrocaloric effect in PbMg0.5W0.5O3 antiferroelectric ceramic. Adv Funct Mater 2021;131:2101176.

Journal of Materiomics
Pages 502-509
Cite this article:
Huang X-X, Ge P-Z, Zhang T-F, et al. Composition-tailor induced electrocaloric effect near room temperature in (Pb,Ba)HfO3 films. Journal of Materiomics, 2023, 9(3): 502-509. https://doi.org/10.1016/j.jmat.2022.12.002

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Received: 11 October 2022
Revised: 03 December 2022
Accepted: 08 December 2022
Published: 29 December 2022
© 2022 The Authors.

This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/).

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