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首页> 外文期刊>Ultrasonics, Ferroelectrics and Frequency Control, IEEE Transactions on >Electric-field and stress effects on depoling and overpoling phenomena in [001]-poled transverse mode pb(zn1/3nb2/3)o3-(6-7)%pbtio3 single crystal of [110] length cut
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Electric-field and stress effects on depoling and overpoling phenomena in [001]-poled transverse mode pb(zn1/3nb2/3)o3-(6-7)%pbtio3 single crystal of [110] length cut

机译:电场和应力对[110]长度切割的[001]极化横向模式pb(zn1 / 3nb2 / 3)o3-(6-7)%pbtio3单晶中的极化和超极化现象的影响

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Solid-solution Pb(Zn1/3Nb2/3)O3-PbTiO3 (PZNPT) single crystals, touted as next-generation piezoelectric materials, have been studied extensively in the past decade. This work addresses the advantages and limitations of transducers made of transverse mode PZN-(6-7)%PT single crystals of [110]L X [001]T(P) cut. This cut exhibits superior electromechanical properties, with k31 Ȥ8; 0.85 and d31 Ȥ8;-1450 pC/N, and an extremely high d31/ SE11 value of >35 C/m2. It also has relatively high overpoling, i.e., rhombohedralto- tetragonal phase transformation, field of Ȥ8;2 kV/mm. This overpoling field further decreases with increase in axial compressive stress. Despite these good attributes, this crystal cut has a low depoling field of ʧD; 0.3 kV/mm, a result of low coercive fields of [001]-poled relaxor-based single crystals, which decreases further with increasing axial compressive stress, limiting its bipolar drive capability. The axial compressive stress required to cause overpoling via rhombohedral-to-tetragonal phase transformation of relevant domain variants in the crystal is found to be >90 MPa. In contrast, this crystal cut depolarizes at comparatively low axial tensile stress of Ȥ8;15 MPa, the magnitude of which is not significantly affected by the moderate forward field applied.
机译:在过去的十年中,对固溶体Pb(Zn1 / 3Nb2 / 3)O3-PbTiO3(PZNPT)单晶进行了广泛的研究。这项工作解决了由[110] L X [001] T(P)切割的横向模式PZN-(6-7)%PT单晶制成的换能器的优点和局限性。该切口具有优异的机电性能,k31Ȥ8; 0.85和d31Ȥ8; -1450 pC / N,并且d31 / SE11的极高值> 35 C / m2。它还具有较高的超标度,即菱面体到四方相变,电场为Ȥ8; 2 kV / mm。随着轴向压缩应力的增加,该外推场进一步减小。尽管具有这些良好的属性,但这种晶体切割的ʧD场低; 0.3 kV / mm是[001]极化弛豫基单晶矫顽场低的结果,随着轴向压缩应力的增加,矫顽场进一步降低,从而限制了其双极驱动能力。发现通过晶体中相关域变体的菱形到四方相变引起超极化所需的轴向压缩应力> 90 MPa。相反,该晶体切割在相对较低的轴向拉伸应力stress8; 15 MPa时去极化,其大小不受所施加的适度正向电场的影响。

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