X-ray and neutron diffraction investigations of the structural phase transformation sequence under electric field in 0.7Pb(Mg1/3Nb2/3)-0.3PbTiO3 crystal
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作者:
Bai, FM
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Virginia Tech, Dept Mat Sci & Engn, Blacksburg, VA 24061 USAVirginia Tech, Dept Mat Sci & Engn, Blacksburg, VA 24061 USA
Bai, FM
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Wang, NG
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机构:Virginia Tech, Dept Mat Sci & Engn, Blacksburg, VA 24061 USA
Wang, NG
Li, JF
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机构:Virginia Tech, Dept Mat Sci & Engn, Blacksburg, VA 24061 USA
Li, JF
Viehland, D
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机构:Virginia Tech, Dept Mat Sci & Engn, Blacksburg, VA 24061 USA
Viehland, D
Gehring, PM
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机构:Virginia Tech, Dept Mat Sci & Engn, Blacksburg, VA 24061 USA
Gehring, PM
Xu, GY
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机构:Virginia Tech, Dept Mat Sci & Engn, Blacksburg, VA 24061 USA
Xu, GY
Shirane, G
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机构:Virginia Tech, Dept Mat Sci & Engn, Blacksburg, VA 24061 USA
Shirane, G
机构:
[1] Virginia Tech, Dept Mat Sci & Engn, Blacksburg, VA 24061 USA
[2] NIST, Ctr Neutron Res, Gaithersburg, MD 20899 USA
[3] Brookhaven Natl Lab, Dept Phys, Upton, NY 11973 USA
The structural phase transformations of 0.7Pb(Mg1/3Nb2/3)O-3-0.3PbTiO(3) (PMN-30%PT) have been studied using x-ray diffraction (XRD) and neutron scattering as a function of temperature and electric field. We observe the phase transformational sequence (i) cubic (C)--> tetragonal (T)--> rhombohedral (R) in the zero-field-cooled (ZFC) condition; (ii) C-->T--> monoclinic (M-C)--> monoclinic (M-A) in the field-cooled (FC) condition; and (iii) R-->M-A-->M-C-->T with increasing field at fixed temperature beginning from the ZFC condition. Upon removal of the field, the M-A phase is stable at room temperature in the FC condition, and also in the ZFC condition with increasing field. Several subtleties of our findings are discussed based on results from thermal expansion and dielectric measurements, including (i) the stability of the M-A phase, (ii) a difference in lattice parameters between inside bulk and outside layer regions, and (iii) a difference in the phase transition temperature between XRD and dielectric data. (C) 2004 American Institute of Physics.