The technologically important frequency
range for the application
of electrostrictors and piezoelectrics is tens of Hz to tens of kHz.
Sm
3+
- and Gd
3+
-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
(RE
0.1
Ce
0.9
O
1.95
, 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 (|
M
33
|) was 10
2
to 10
4
-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.