Trivalent Dopant Size Influences Electrostrictive Strain in Ceria Solid Solutions

Maxim Varenik, Juan Claudio Nino, Ellen Wachtel, Sangtae Kim, Sidney Cohen, Igor Lubomirsky*

*Corresponding author for this work

Research output: Contribution to journalArticlepeer-review

13 Citations (Scopus)

Abstract

The technologically important frequency range for the application of electrostrictors and piezoelectrics is tens of Hz to tens of kHz. Sm3+- and Gd3+-doped ceria ceramics, excellent intermediate-temperature ion conductors, have been shown to exhibit very large electrostriction below 1 Hz. Why this is so is still not understood. While optimal design of ceria-based devices requires an in-depth understanding of their mechanical and electromechanical properties, systematic investigation of the influence of dopant size on frequency response is lacking. In this report, the mechanical and electromechanical properties of dense ceria ceramics doped with trivalent lanthanides (RE0.1Ce0.9O1.95, RE = Lu, Yb, Er, Gd, Sm, and Nd) were investigated. Young’s, shear, and bulk moduli were obtained from ultrasound pulse echo measurements. Nanoindentation measurements revealed room-temperature creep in all samples as well as the dependence of Young’s modulus on the unloading rate. Both are evidence for viscoelastic behavior, in this case anelasticity. For all samples, within the frequency range f = 0.15–150 Hz and electric field E ≤ 0.7 MV/m, the longitudinal electrostriction strain coefficient (|M33|) was 102 to 104-fold larger than expected for classical (Newnham) electrostrictors. However, electrostrictive strain in Er-, Gd-, Sm-, and Nd-doped ceramics exhibited marked frequency relaxation, with the Debye-type characteristic relaxation time τ ≤ 1 s, while for the smallest dopants—Lu and Yb—little change in electrostrictive strain was detected over the complete frequency range studied. We find that only the small, less-studied dopants continue to produce useable electrostrictive strain at the higher frequencies. We suggest that this striking difference in frequency response may be explained by postulating that introduction of a dopant induces two types of polarizable elastic dipoles and that the dopant size determines which of the two will be dominant.
Original languageEnglish
Pages (from-to)20269-20276
Number of pages8
JournalACS applied materials & interfaces
Volume13
Issue number17
Early online date22 Apr 2021
DOIs
Publication statusPublished - 5 May 2021

Funding

This work is made possible in part by the historic generosity of the Harold Perlman Family. This work was supported in part by the BioWings project, which has received funding from the European Union’s Horizon 2020 under the Future and Emerging Technologies (FET) program with grant agreement no. 801267, and by the U.S.–Israel Binational Science Foundation (2016006). I.L. expresses gratitude to the Estate of Olga Klein—Astrachan fund (#721977).

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