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首页> 外文期刊>Journal of Applied Physics >Electric-field-induced orthorhombic to rhombohedral phase transition in [111]_c-oriented 0.92Pb(Zn_(1/3)Nb_(2/3))O_3-0.08PbTiO_3
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Electric-field-induced orthorhombic to rhombohedral phase transition in [111]_c-oriented 0.92Pb(Zn_(1/3)Nb_(2/3))O_3-0.08PbTiO_3

机译:电场诱导的[111] _c取向的0.92Pb(Zn_(1/3)Nb_(2/3))O_3-0.08PbTiO_3的正交晶向菱面体相变

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摘要

Strain-field measurements and in situ polarized light microscopy have been used to evidence a hysteretic, irreversible electric-field-induced transition to a quasimonodomain rhombohedral phase in [111]_c-oriented, pseudo-orthorhombic PZN-8PT [0.92Pb(Zn_(1/3)Nb_(2/3))O_3-0.08PbTiO_3]. This first-order transition most likely occurs following the simplest path O-M_B-R, i.e., via polarization rotation in the (10-l)_c plane. The measured strain-field loops are compared to those for rhombohedral, [111]_c-oriented PMN-28PT [0.72Pb(Mg_(1/3)Nb_(2/3))O_3-0.28PbTiO_3] and PMN -33PT [0.67Pb(Mg_(1/3)Nb_(2/3))O_3-0.33PbTiO_3] where no electric-field-induced transition is possible.
机译:应变场测量和原位偏振光显微镜已被用来证明在[111] _c取向的拟斜方PZN-8PT [0.92Pb(Zn_( 1/3)Nb_(2/3))O_3-0.08PbTiO_3]。该一阶跃迁最有可能沿着最简单的路径O-M_B-R发生,即通过(10-1)_c平面中的极化旋转。将测得的应变场回路与菱形,面向[111] _c的PMN-28PT [0.72Pb(Mg_(1/3)Nb_(2/3))O_3-0.28PbTiO_3]和PMN -33PT [0.67]比较Pb(Mg_(1/3)Nb_(2/3))O_3-0.33PbTiO_3],其中电场诱导的跃迁是不可能的。

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