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Excellent hardening effect in lead-free piezoceramics by embedding local Cu-doped defect dipoles in phase boundary engineering

Xinyue Qiu, Chao Wu, Daniel Q. Tan (), Ruihong Liang, Chen Liu, Yinchang Ma, Xi-xiang Zhang, Shiyang Wei, Junwei Zhang, Zhi Tan, Zhipeng Wang (), Xiang Lv () and Jiagang Wu ()
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Xinyue Qiu: Sichuan University
Chao Wu: Sichuan University
Daniel Q. Tan: Guangdong Technion-Israel Institute of Technology
Ruihong Liang: Chinese Academy of Sciences
Chen Liu: King Abdullah University of Science and Technology
Yinchang Ma: King Abdullah University of Science and Technology
Xi-xiang Zhang: King Abdullah University of Science and Technology
Shiyang Wei: Lanzhou University
Junwei Zhang: Lanzhou University
Zhi Tan: Sichuan University
Zhipeng Wang: Xidian University
Xiang Lv: Sichuan University
Jiagang Wu: Sichuan University

Nature Communications, 2025, vol. 16, issue 1, 1-11

Abstract: Abstract Piezoceramics for high-power applications require both high piezoelectric coefficient (d33) and mechanical quality factor (Qm). However, the trade-off between them poses a significant challenge in achieving high values simultaneously, which is more prominent in lead-free piezoceramics. Here, we propose a new strategy, local Cu-acceptor defect dipoles embedded orthorhombic-tetragonal phase boundary engineering (O-T PBE), to balance d33 and Qm in potassium sodium niobate piezoceramics. This is validated in 0.95(K0.48Na0.52)NbO3-0.05(Bi0.5Na0.5)HfO3-0.2%molFe2O3-xmol%CuO ceramics. Our strategy simultaneously maintains the O-T PBE and introduces local dimeric $${({{Cu}}_{{Nb}}^{{\prime} {\prime} {\prime} }-{V}_{O}^{\bullet \bullet })}^{{\prime} }$$ ( C u N b ″ ′ − V O ∙ ∙ ) ′ and trimeric $${\left({V}_{O}^{\bullet \bullet }-{{Cu}}_{{Nb}}^{{\prime} {\prime} {\prime} }-{V}_{O}^{\bullet \bullet }\right)}^{\bullet }$$ V O ∙ ∙ − C u N b ″ ′ − V O ∙ ∙ ∙ defects. The dimeric defects form defect dipole polarization that pins domain wall motion, while the trimeric ones introduce the local structural heterogeneity that leads to nano-scale multi-phase coexistence and abundant nano-domains. Encouragingly, for the Cu-doped sample with x = 1, Qm increases by a factor of 4, but d33 only decreases by 1/5 (i.e., achieving a d33 of 340 pC/N and a Qm of 256). Our research provides a new paradigm for balancing d33 and Qm in lead-free piezoceramics, which holds promise for high-power applications.

Date: 2025
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DOI: 10.1038/s41467-025-58269-5

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