TY - JOUR
T1 - Landau expansion parameters and the O-T phase transition of a 0.64Pb(M g1/3 N b2/3) O3-0.36PbTi O3 single crystal
AU - Zhang, Hangbo
AU - Lu, Xiaoyan
AU - Wang, Chunying
AU - Zheng, Limei
AU - Yang, Bin
AU - Cao, Wenwu
N1 - Funding Information:
This research was supported by the National Natural Science Foundation of China (Grants No. 11372002 and No. 51572055), the National Key Basic Research Program of China (Grant No. 2013CB632900), and the PIRS of HIT (Grant No. B201509).
Publisher Copyright:
© 2018 American Physical Society.
PY - 2018/2/28
Y1 - 2018/2/28
N2 - Landau free-energy expansion parameters for 0.64Pb(Mg1/3Nb2/3)O3-0.36PbTiO3 single crystal were determined from the temperature-dependent polarization-electric field (P-E) hysteresis loops along [001]C, the temperature-dependent dielectric constant 11, and the electric-field-induced tetragonal-rhombohedral phase-transition temperature. Using these obtained parameters, the phase-transition behavior, polarization, dielectric, and piezoelectric constants can all be calculated, which showed good agreement with experimental results. An orthorhombic-to-tetragonal phase transition was predicted to be around -15°C, near which coexisting orthorhombic phase and tetragonal phase were confirmed by experiments. Based on our calculations, we concluded that the commonly observed monoclinic phase around the orthorhombic-to-tetragonal phase-transition temperature was an adaptive structure due to the coexistence of tetragonal and orthorhombic phases. Additionally, large shear piezoelectric responses exist near room temperature due to the instability caused by the competition between the coexisting tetragonal and orthorhombic phases.
AB - Landau free-energy expansion parameters for 0.64Pb(Mg1/3Nb2/3)O3-0.36PbTiO3 single crystal were determined from the temperature-dependent polarization-electric field (P-E) hysteresis loops along [001]C, the temperature-dependent dielectric constant 11, and the electric-field-induced tetragonal-rhombohedral phase-transition temperature. Using these obtained parameters, the phase-transition behavior, polarization, dielectric, and piezoelectric constants can all be calculated, which showed good agreement with experimental results. An orthorhombic-to-tetragonal phase transition was predicted to be around -15°C, near which coexisting orthorhombic phase and tetragonal phase were confirmed by experiments. Based on our calculations, we concluded that the commonly observed monoclinic phase around the orthorhombic-to-tetragonal phase-transition temperature was an adaptive structure due to the coexistence of tetragonal and orthorhombic phases. Additionally, large shear piezoelectric responses exist near room temperature due to the instability caused by the competition between the coexisting tetragonal and orthorhombic phases.
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U2 - 10.1103/PhysRevB.97.054114
DO - 10.1103/PhysRevB.97.054114
M3 - Article
AN - SCOPUS:85043788113
SN - 2469-9950
VL - 97
JO - Physical Review B
JF - Physical Review B
IS - 5
M1 - 054114
ER -