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Piezoelectric and Ferroelectric Materials

A special issue of Materials (ISSN 1996-1944). This special issue belongs to the section "Materials Physics".

Deadline for manuscript submissions: closed (20 September 2023) | Viewed by 2297

Special Issue Editors


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Guest Editor
College of Materials and Metallurgy, Guizhou University, Guiyang 550025, China
Interests: piezoelectric and ferroelectric materials
College of Materials and Metallurgy, Guizhou University, Guiyang 550025, China
Interests: microporous and mesoporous zeolite; zeolite membrane

Special Issue Information

Dear Colleagues,

The last two decades have witnessed the rapid development of piezoelectric and ferroelectric materials, which are widely utilized as sensors, actuators, high-performance capacitors, diverse dimension functional composites, etc. A material design employing component modulation and microstructure construction and preparation technique exploration promote the performances of such materials. Additionally, with recent advances in functionalization and integration research, the exploitation of more applications for piezoelectric and ferroelectric materials is further being boosted.

To show the development of materials and their in-depth exploitation, it is necessary to extensively investigate the materials from the perspectives of the material system, material scale, material microstructure, and application.

The main synthesis methods include hydrothermal synthesis, microwave synthesis, seed crystal synthesis, ultrasonic synthesis, template method, confined space synthesis, etc. With the continued development of materials, synthesis techniques have become more abundant.

Dr. Yuanyu Wang
Dr. Qi Sun
Guest Editors

Manuscript Submission Information

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Keywords

  • piezoelectric
  • ferroelectric
  • bulk material
  • low-dimension material
  • functionalization
  • integration
  • applications

Published Papers (2 papers)

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Research

15 pages, 3462 KiB  
Article
Exploring the BiFeO3-PbTiO3-SrTiO3 Ternary System to Obtain Good Piezoelectrical Properties at Low and High Temperatures
by Anton Tuluk and Sybrand van der Zwaag
Materials 2023, 16(21), 6840; https://doi.org/10.3390/ma16216840 - 24 Oct 2023
Viewed by 727
Abstract
In this work, we investigated the piezoelectric properties of BiFeO3-rich (1 − (y + x)) BiFeO3–y PbTiO3–x SrTiO3 (0.1 ≤ x ≤ 0.35; 0.1 ≤ y ≤ 0.3) bulk piezoceramics, as this system could potentially lead [...] Read more.
In this work, we investigated the piezoelectric properties of BiFeO3-rich (1 − (y + x)) BiFeO3–y PbTiO3–x SrTiO3 (0.1 ≤ x ≤ 0.35; 0.1 ≤ y ≤ 0.3) bulk piezoceramics, as this system could potentially lead to the development of bulk piezoelectric ceramics that are suitable for high-temperature applications (>200 °C). Samples with various levels of PbTiO3 and SrTiO3 were prepared via a conventional solid-state route. X-ray diffraction confirmed a pure perovskite phase for the compositions, which was explored without secondary phases. It was found that the addition of comparable levels of PbTiO3 and SrTiO3 to the BiFeO3 ceramic resulted in higher piezoelectric properties compared to those of the pure BiFeO3 and binary systems. The Curie temperature was significantly reduced by dual doping, with SrTiO3 and PbTiO3 additions resulting in comparable Curie temperature depressions. The locations of the phase boundaries between the cubic, pseudocubic, and rhombohedral crystal structures were determined. The highest piezoelectric properties, including a d33 value of 250 pC/N at room temperature, were obtained for the samples with the composition x = 0.3, y = 0.25, which was close to the cubic–pseudocubic phase boundary in the phase diagram. The temperature dependence of the piezoelectric properties varied depending on the previous thermal history, yet an appropriate heat treatment resulted in an almost temperature-stable d33 value. The ceramic with the lowest temperature sensitivity and a high Curie temperature of 350 °C was found for x = 0.1, y = 0.2 with a d33 value of 60 pC/N at RT and 71 pC/N at 300 °C (after poling at 60 kV/cm and a stabilizing heat treatment). However, the materials developed were still unsuitable for applications at high temperatures due to a rapidly increasing electrical conductivity with increasing temperature. Full article
(This article belongs to the Special Issue Piezoelectric and Ferroelectric Materials)
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15 pages, 6959 KiB  
Article
Yttrium and Niobium Elements Co-Doping and the Formation of Double Perovskite Structure Ba2YNbO6 in BCZT
by Runyu Mao, Deyi Zheng, Qiyun Wu, Yuying Wang and Chang Liu
Materials 2023, 16(11), 4044; https://doi.org/10.3390/ma16114044 - 29 May 2023
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Abstract
The (Ba0.85Ca0.15) (Ti0.90Zr0.10)O3 + x Y3+ + x Nb5+ (abbreviated as BCZT-x(Nb + Y), x = 0 mol%, 0.05 mol%, 0.1 mol%, 0.2 mol%, 0.3 mol%) lead-free piezoceramics samples were [...] Read more.
The (Ba0.85Ca0.15) (Ti0.90Zr0.10)O3 + x Y3+ + x Nb5+ (abbreviated as BCZT-x(Nb + Y), x = 0 mol%, 0.05 mol%, 0.1 mol%, 0.2 mol%, 0.3 mol%) lead-free piezoceramics samples were prepared by a traditional solid-state sintering method. And the effects of Yttrium and Niobium elements (Y3+ and Nb5+) co-doping on the defect, phase and structure, microstructure, and comprehensive electrical properties have been investigated. Research results show that the Y and Nb elements co-doping can dramatically enhance piezoelectric properties. It is worth noting that XPS defect chemistry analysis, XRD phase analysis and TEM results together show that a new phase of double perovskite structure Barium Yttrium Niobium Oxide (Ba2YNbO6) is formed in the ceramic, and the XRD Rietveld refinement and TEM results show the coexistence of the R-O-T phase. Both these two reasons together lead to significant performance improvements of piezoelectric constant (d33) and planar electro-mechanical coupling coefficient (kp). The functional relation between temperature and dielectric constant testing results present that the Curie temperature increases slightly, which shows the same law as the change of piezoelectric properties. The ceramic sample reaches an optimal performance at x = 0.1% of BCZT-x(Nb + Y), where d33 = 667 pC/N, kp = 0.58, εr = 5656, tanδ = 0.022, Pr = 12.8 μC/cm2, EC = 2.17 kV/cm, TC =92 °C, respectively. Therefore, they can be used as potential alternative materials to lead based piezoelectric ceramics. Full article
(This article belongs to the Special Issue Piezoelectric and Ferroelectric Materials)
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