Chemical Compensation Challenges in Processing Antiferroelectric PbZrO<sub>3</sub> Thin Films

The electric field-induced antipolar-to-polar phase transition in antiferroelectric materials is accompanied by large changes in the structural and functional response, making them attractive for many applications ranging from pulsed energy capacitors to high-strain-high (blocking-)-force actuators, solid-state heating and cooling systems, and optoelectronic devices. PbZrO<sub>3</sub>, as an end member of the PZT, (<i>x</i>)-PbZr<sub>1-<i>x</i></sub> Ti <sub><i>x</i></sub> O<sub>3</sub>, solid solution, has been the subject of many studies. However, processing of perovskite PbZrO<sub>3</sub> is extremely challenging due to phase instabilities induced by Pb loss at the temperatures necessary for perovskite crystallization. Here, we discuss the challenges associated with Pb loss, as well as its compensation through bulk Pb overstoichiometry and interfacial PbO additions, in chemical solution processed, highly oriented PbZrO<sub>3</sub> thin films. For both 042<sub>o</sub>- and 001<sub>o</sub>-oriented (<i>o</i>-orthorhombic distortion) PbZrO<sub>3</sub> thin films, the crystallization interfaces are the most important contributors to Pb loss and off-stoichiometric outcomes, and no single approach was sufficient to address these challenges. Pb-rich and Pb-deficient nonperovskite phases including ZrO <sub><i>x</i></sub> were only observable through microscopic characterization, and X-ray diffraction alone could not rule out the presence of such secondary phases. "Ideal" macroscopic antiferroelectric polarization-electric field double hysteresis curves were observed despite (at times) the large presence of secondary phases. However, reduced saturation polarization and increased phase transition electric fields were observed concomitantly with the presence of secondary phase(s) and tentatively assigned to the voltage drop across the ZrO <sub><i>x</i></sub> nanocrystals. Based on these results, it is imperative that the presence of secondary phases always be addressed (beyond X-ray diffraction spectra) in order to correctly evaluate the properties of antiferroelectric films.

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Journal
ACS Omega
Published
2025-07-05
DOI
https://doi.org/10.1021/acsomega.5c04818
Primary Topic
Ferroelectric and Piezoelectric Materials
Type
article
Field-Weighted Citation Impact
0.00

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article

Chemical Compensation Challenges in Processing Antiferroelectric PbZrO3 Thin Films

В. А. Лебедев, Lewys Jones, S. Lisenkov, I. Ponomareva et al.
ACS Omega
Ferroelectric and Piezoelectric Materials
article

Chemical Compensation Challenges in Processing Antiferroelectric PbZrO3 Thin Films

В. А. Лебедев, Lewys Jones, S. Lisenkov, I. Ponomareva, Sarah J. Stock, Nazanin Bassiri‐Gharb, Kristina M. Holsgrove, Nikhilesh Maity, Amit Kumar, Milan Haddad, Sergio Rivera-Cruz
article en

Abstract

The electric field-induced antipolar-to-polar phase transition in antiferroelectric materials is accompanied by large changes in the structural and functional response, making them attractive for many applications ranging from pulsed energy capacitors to high-strain-high (blocking-)-force actuators, solid-state heating and cooling systems, and optoelectronic devices. PbZrO<sub>3</sub>, as an end member of the PZT, (<i>x</i>)-PbZr<sub>1-<i>x</i></sub> Ti <sub><i>x</i></sub> O<sub>3</sub>, solid solution, has been the subject of many studies. However, processing of perovskite PbZrO<sub>3</sub> is extremely challenging due to phase instabilities induced by Pb loss at the temperatures necessary for perovskite crystallization. Here, we discuss the challenges associated with Pb loss, as well as its compensation through bulk Pb overstoichiometry and interfacial PbO additions, in chemical solution processed, highly oriented PbZrO<sub>3</sub> thin films. For both 042<sub>o</sub>- and 001<sub>o</sub>-oriented (<i>o</i>-orthorhombic distortion) PbZrO<sub>3</sub> thin films, the crystallization interfaces are the most important contributors to Pb loss and off-stoichiometric outcomes, and no single approach was sufficient to address these challenges. Pb-rich and Pb-deficient nonperovskite phases including ZrO <sub><i>x</i></sub> were only observable through microscopic characterization, and X-ray diffraction alone could not rule out the presence of such secondary phases. "Ideal" macroscopic antiferroelectric polarization-electric field double hysteresis curves were observed despite (at times) the large presence of secondary phases. However, reduced saturation polarization and increased phase transition electric fields were observed concomitantly with the presence of secondary phase(s) and tentatively assigned to the voltage drop across the ZrO <sub><i>x</i></sub> nanocrystals. Based on these results, it is imperative that the presence of secondary phases always be addressed (beyond X-ray diffraction spectra) in order to correctly evaluate the properties of antiferroelectric films.

ACS OmegaVol. 10(27)
Queen's University Belfast (GB), Georgia Institute of Technology (US), Trinity College Dublin (IE), University of South Florida (US), University of Puerto Rico-Mayaguez (PR)
Georgia Institute of Technology, Department of Education and Learning, Northern Ireland, Science Foundation Ireland, Division of Materials Research, Division of Electrical, Communications and Cyber Systems, Basic Energy Sciences
Openalex Percentile: Top 89%
Ferroelectric and Piezoelectric Materials
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