TY - JOUR
T1 - Effect of stresses on the dielectric and piezoelectric properties of Pb(Zr0.52Ti0.48)O3 thin films
AU - Coleman, K.
AU - Walker, J.
AU - Beechem, T.
AU - Trolier-Mckinstry, S.
N1 - Funding Information:
Sandia National Laboratories is a multimission laboratory managed and operated by National Technology and Engineering Solutions of Sandia, LLC, a wholly owned subsidiary of Honeywell International Inc., for the U.S. Department of Energy’s (DOE) National Nuclear Security Administration under Contract No. DE-NA0003525.
Funding Information:
This manuscript is based on the work supported by the National Science Foundation (NSF) as part of the Center for Dielectrics and Piezoelectrics under Grant Nos. IIP-1361571 and IIP-1361503.
Publisher Copyright:
© 2019 Author(s).
PY - 2019/7/21
Y1 - 2019/7/21
N2 - Flexible piezoelectric microelectromechanical systems can experience a wide range of stress conditions. In order to explore the functional properties over this range, the dielectric and piezoelectric properties of 0.6 μm thick {001} sol-gel Pb0.99⧠0.01(Zr0.52Ti0.48)0.98Nb0.02O3 (PZT) films on Si substrates and thin Ni foils were measured as a function of stress arising from thermal expansion mismatch during fabrication or applied by bending of a cantilever. Due to the differences in residual thermal stress, the remanent polarization, Pr, was approximately 21 ± 0.2 μC/cm2 and 39.5 ± 2.3 μC/cm2 for PZT films on Si and Ni, respectively, with the higher Pr on Ni originating from more "c" domains (out-of-plane polarization) due to the compressive stresses. The link between stress and domain orientation was further explored by bending films on Ni around mandrels with known radii of curvature to apply uniaxial strains of -0.2% to 0.5%. Films on Si were only exposed to strains between -0.06% and 0.06%, because of substrate failure. For films on 50 μm thick Ni foil, under a 0.5% tensile strain, the Pr decreased by 7%-10% and the permittivity increased up to 23% relative to zero applied stress samples. This trend reversed upon compressive strain. In addition, the piezoelectric coefficient, e31,f, is reported to be -9.0 ± 0.45 μC/cm2 and -7.1 ± 0.35 μC/cm2 on Ni and Si, respectively, and increased in magnitude with applied uniaxial compressive strain. These changes are consistent with substantial levels of ferroelastic reorientation.
AB - Flexible piezoelectric microelectromechanical systems can experience a wide range of stress conditions. In order to explore the functional properties over this range, the dielectric and piezoelectric properties of 0.6 μm thick {001} sol-gel Pb0.99⧠0.01(Zr0.52Ti0.48)0.98Nb0.02O3 (PZT) films on Si substrates and thin Ni foils were measured as a function of stress arising from thermal expansion mismatch during fabrication or applied by bending of a cantilever. Due to the differences in residual thermal stress, the remanent polarization, Pr, was approximately 21 ± 0.2 μC/cm2 and 39.5 ± 2.3 μC/cm2 for PZT films on Si and Ni, respectively, with the higher Pr on Ni originating from more "c" domains (out-of-plane polarization) due to the compressive stresses. The link between stress and domain orientation was further explored by bending films on Ni around mandrels with known radii of curvature to apply uniaxial strains of -0.2% to 0.5%. Films on Si were only exposed to strains between -0.06% and 0.06%, because of substrate failure. For films on 50 μm thick Ni foil, under a 0.5% tensile strain, the Pr decreased by 7%-10% and the permittivity increased up to 23% relative to zero applied stress samples. This trend reversed upon compressive strain. In addition, the piezoelectric coefficient, e31,f, is reported to be -9.0 ± 0.45 μC/cm2 and -7.1 ± 0.35 μC/cm2 on Ni and Si, respectively, and increased in magnitude with applied uniaxial compressive strain. These changes are consistent with substantial levels of ferroelastic reorientation.
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U2 - 10.1063/1.5095765
DO - 10.1063/1.5095765
M3 - Article
AN - SCOPUS:85069497368
SN - 0021-8979
VL - 126
JO - Journal of Applied Physics
JF - Journal of Applied Physics
IS - 3
M1 - 034101
ER -