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Current Applied Materials

Editor-in-Chief

ISSN (Print): 2666-7312
ISSN (Online): 2666-7339

Research Article

Pure PZT95/5 Ceramics and Its Phase Transition Behavior Under External Fields

Author(s): Hengchang Nie*, Fei Cao, Genshui Wang and Xianlin Dong

Volume 1, Issue 1, 2022

Published on: 05 July, 2021

Article ID: e050821194453 Pages: 6

DOI: 10.2174/2666731201666210705100828

Abstract

Background: Compositionally modified Pb(Zr0.95Ti0.05)O3 (PZT 95/5) ferroelectric materials have been extensively investigated in past decades for many important applications. However, few study on pure PZT95/5 ceramics have been reported.

Objective: Herein, pure PZT95/5 ceramics were successfully prepared, and their microstructure and phase transition behaviors under external fields were studied.

Methods: The pure PZT95/5 ceramics were prepared by the conventional solid state reaction using a mixed oxide route. The microstructure and its properties under different external fields were measured.

Results: The X-ray diffraction patterns indicated that the virgin pure PZT95/5 ceramics exhibit an orthorhombic antiferroelectric phase, which has also been evidenced by the superlattice reflections in the SAED pattern. While a rhombohedral ferroelectric symmetry crystal structure was observed in the poled samples suggesting that an electric field induced antiferroelectric to ferroelectric phase transition takes place. Pure PZT95/5 ceramics exhibit a quenched ferroelectric hysteresis loop with a remnant polarization of ~8μC/cm2 under 3.5kV/mm. Temperature dependence dielectric response indicated that the orthorhombic antiferroelectric to cubic paraelectric phase transition occurs at 225°C, corresponding to its Curie temperature. A shard depolarization behavior and dielectric anomalies were observed under ~240 MPa hydrostatic pressure.

Conclusion: The depolarization mechanism of pure PZT95/5 ceramics under hydrostatic pressure is attributed to the hydrostatic pressure-induced FE-AFE phase transition. These results will offer fundamental insights into PZT95/5 ceramics for pulsed power supply applications.

Keywords: PZT95/5, antiferroelectric, phase transition, pulsed power supply, depolarization behavior, hydrostatic pressure.

Graphical Abstract

[1]
Mischenko AS, Zhang Q, Scott JF, Whatmore RW, Mathur ND. Giant electrocaloric effect in thin-film PbZr(0.95)Ti(0.05)O3. Science 2006; 311(5765): 1270-1.
[http://dx.doi.org/10.1126/science.1123811] [PMID: 16513978]
[2]
Hao X, Yue Z, Xu J, et al. Energy-storage performance and electrocaloric effect in (100)-oriented Pb0.97La0.02(Zr0.95Ti0.05)O3 antiferroelectric thick films. J Appl Phys 2011; 110: 064109.
[http://dx.doi.org/10.1063/1.3641983]
[3]
Ge J, Dong XL, Chen Y, et al. Enhanced polarization switching and energy storage properties of Pb0.97La0.02(Zr0.95Ti0.05)O3 antiferroelectric thin films with LaNiO3 oxide top electrodes. Appl Phys Lett 2013; 102: 142905.
[http://dx.doi.org/10.1063/1.4801517]
[4]
Liu QX, Tang XG, Jiang YP, et al. Ferroelectric and pyroelectric properties of highly (111)-oriented nanocrystalline Pb(Zr0.95Ti0.05)O3 thin films. Chin J Chem Phys 2007; 20: 763-7.
[http://dx.doi.org/10.1088/1674-0068/20/06/763-767]
[5]
Dong XL, Kojima S. Dielectric and resonance frequency investigations of phase transitions in Nb-doped PZT95/5 and 75/25 ceramics. J Phys Condens Matter 1997; 9: L171-7.
[http://dx.doi.org/10.1088/0953-8984/9/11/003]
[6]
Setchell RE. Shock wave compression of the ferroelectric ceramic Pb0.99(Zr0.95Ti0.05)0.98Nb0.02O3: Hugoniot states and constitutive mechanical properties. J Appl Phys 2003; 94: 573-88.
[http://dx.doi.org/10.1063/1.1578526]
[7]
Nie H, Yu Y, Liu Y, et al. Enhanced shock performance by disperse porous structure: A case study in PZT95/5 ferroelectric ceramics. J Am Ceram Soc 2017; 100: 5693-9.
[http://dx.doi.org/10.1111/jace.15097]
[8]
Dong Wen D, Valadez J. Carlos, and Lynch Christopher S., Pressure, temperature, and electric field dependence of phase transformations in niobium modified 95/5 lead zirconate titanate. J Appl Phys 2015; 117: 244104.
[http://dx.doi.org/10.1063/1.4923036]
[9]
Neilson FW. Effects of strong shocks in ferroelectric materials. Bull Am Phys Soc 1957; 2: 302.
[10]
Dungan RH, Storz LJ. Relation between chemical, mechanical, and electrical properties of Nb2O5-modified 95 mol% PbZrO3-5mol% PbTiO3. J Am Ceram Soc 1985; 68: 530-3.
[http://dx.doi.org/10.1111/j.1151-2916.1985.tb11518.x]
[11]
Tuttle BA, Yang P, Gieske JH, et al. Pressure-induced phase transformation of controlled-porosity Pb(Zr0.95Ti0.05)O3 ceramics. J Am Ceram Soc 2001; 84(1260-1264)
[http://dx.doi.org/10.1111/j.1151-2916.2001.tb00826.x]
[12]
Valadez JC, Sahul R, Lynch CS. The effect of a hydrostatic pressure induced phase transformation on the unipolar electrical response of Nb modified 95/5 lead zirconate titanate. J Appl Phys 2012; 111: 024109.
[http://dx.doi.org/10.1063/1.3677980]
[13]
Shkuratov SI, Baird J, Antipov VG, et al. Depolarization mechanisms of PbZr0.52Ti0.48O3 and PbZr0.95Ti0.05O3 poled ferroelectrics under high strain rate loading. Appl Phys Lett 2014; 104: 212901.
[http://dx.doi.org/10.1063/1.4879545]
[14]
Shkuratov SI, Baird J, Talantsev EF. Note: Utilizing Pb(Zr(0.95)Ti(0.05))O3 ferroelectric ceramics to scale down autonomous explosive-driven shock-wave ferroelectric generators. Rev Sci Instrum 2012; 83(7): 076104.
[http://dx.doi.org/10.1063/1.4733294] [PMID: 22852739]
[15]
Zhang FP, Liu YS, Xie QH, et al. Electrical response of Pb(Zr0.95Ti0.05)O3 under shock compressions. J Appl Phys 2015; 117: 134104.
[http://dx.doi.org/10.1063/1.4916710]
[16]
Jiang D, Du J, Gu Y, et al. Self-generated electric field suppressing the ferroelectric to antiferroelectric phase transition in ferroelectric ceramics under shock wave compression. J Appl Phys 2012; 111: 024103.
[http://dx.doi.org/10.1063/1.3678005]
[17]
Zhang Q, Whatmore RW. Improved ferroelectric and pyroelectric properties in Mn-doped lead zirconate titanate thin films. J Appl Phys 2003; 94: 5228-33.
[http://dx.doi.org/10.1063/1.1613370]
[18]
Zhang S, Li F. High performance ferroelectric relaxor-PbTiO3 single crystals: status and perspective. J Appl Phys 2012; 111: 031301.
[http://dx.doi.org/10.1063/1.3679521]
[19]
Tan Q, Xu Z, Viehland D. Effect of substituents with different valences on antiferroelectric stability of antiferroelectric lead zirconate ceramics. J Mater Res 1999; 14: 4251-8.
[http://dx.doi.org/10.1557/JMR.1999.0576]
[20]
Taylor GW. Electrical Properties of Niobium-Doped Ferroelectric Pb(Zr, Sn, Ti)O3 Ceramics. J Appl Phys 1967; 38: 4696.
[http://dx.doi.org/10.1063/1.1709206]
[21]
Gerson R. Variation in ferroelectric characteristics of lead zirconate titanate ceramics due to minor chemical modifications. J Appl Phys 1960; 31: 188.
[http://dx.doi.org/10.1063/1.1735397]
[22]
Sawaguchi E. Ferroelectric versus antiferroelectric in the solid solutions of PbZrO3 and PbTiO3. J Phys Soc Jpn 1953; 1078: 615-29.
[http://dx.doi.org/10.1143/JPSJ.8.615]
[23]
Jona F, Shirane G, Mazzi F, Pepinsky R. X-ray and neutron diffraction study of antiferroelectric lead zirconate PbZrO3. Phys Rev 1957; 105: 849-56.
[http://dx.doi.org/10.1103/PhysRev.105.849]
[24]
Viehland D. Transmission electron microscopy study of high-Zr-content lead zirconate titanate. Phys Rev B Condens Matter 1995; 52(2): 778-91.
[http://dx.doi.org/10.1103/PhysRevB.52.778] [PMID: 9980653]
[25]
Nie HC, Feng NB, Chen XF, Wang GS, Dong XL, Gu Y. Enhanced ferroelectric properties of intragranular-porous Pb(Zr0.95Ti0.05)O3 ceramic fabricated with carbon nanotubes. J Am Ceram Soc 2010; 93: 642-5.
[http://dx.doi.org/10.1111/j.1551-2916.2009.03479.x]
[26]
Jiang Z, Shen H, Xin M, et al. Mechanical properties and depoling of porous poled PZT95/5 ferroelectric ceramics under uniaxial compression. Chin J Solid Mech 2016; 37(1): 50-8.
[http://dx.doi.org/10.3390/ma13214730]
[27]
Whatmore RW, Clarke R, Glazer AM. Tricritical behaviour in PbZrxTi1-xO3 solid solutions. J Phys C Solid State Phys 1978; 11: 3089.
[http://dx.doi.org/10.1088/0022-3719/11/14/029]
[28]
Nie H, Dong X, Chen X, et al. Tailored electrical properties with enhanced fracture toughness in Pb0.99(Zr0.95Ti0.05)0.98Nb0.02O3 ferroelectric ceramics. Mater Res Bull 2013; 48: 3088-91.
[http://dx.doi.org/10.1016/j.materresbull.2013.04.049]
[29]
Samara GA, Venturini EL, Yang P. Pressure-induced ferroelectric to antiferroelectric phase transition in Pb0.99(Zr0.95Ti0.05)0.98Nb0.02O3. Phys Rev B Condens Matter Mater Phys 2006; 73: 064105.
[http://dx.doi.org/10.1103/PhysRevB.73.064105]
[30]
Hall DA, Evans JDS, Covey-Crump SJ. Effects of superimposed electric field and porosity on the hydrostatic pressure-induced rhombohedral to orthorhombic martensitic phase transformation in PZT 95/5 ceramics. Acta Mater 2010; 58: 6584-91.
[http://dx.doi.org/10.1016/j.actamat.2010.07.032]

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