首页> 外文期刊>Journal of Applied Physics >The morphotropic phase boundary and dielectric properties of the xPb(Zr1/2Ti1/2)O-3-(1-x)Pb(Ni1/3Nb2/3)O-3 perovskite solid solution
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The morphotropic phase boundary and dielectric properties of the xPb(Zr1/2Ti1/2)O-3-(1-x)Pb(Ni1/3Nb2/3)O-3 perovskite solid solution

机译:xPb(Zr1 / 2Ti1 / 2)O-3-(1-x)Pb(Ni1 / 3Nb2 / 3)O-3钙钛矿固溶体的相变相界和介电性质

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The solid solution between the normal ferroelectric Pb(Zr1/2Ti1/2)O-3 (PZT) and relaxor ferroelectric Pb(Ni1/3Nb2/3)O-3 (PNN) was synthesized by the columbite method. The phase structure and dielectric properties of xPZT-(1-x)PNN where x=0.4-0.9 and the Zr/Ti composition was fixed close to the morphotropic phase boundary (MPB) were investigated. With these data, the ferroelectric phase diagram between PZT and PNN has been established. The relaxor ferroelectric nature of PNN gradually transformed towards a normal ferroelectric state towards the composition 0.7PZT-0.3PNN, in which the permittivity was characterized by a sharp peak and the disappearance of dispersive behavior. X-ray diffraction analysis demonstrated the coexistence of both the rhombohedral and tetragonal phases at the composition 0.8PZT-0.2PNN, a new morphotropic phase boundary within this system. Examination of the dielectric spectra indicates that PZT-PNN exhibits an extremely high relative permittivity near the MPB composition. The permittivity shows a shoulder at the rhombohedral to tetragonal phase transition temperature T-RT=195 degreesC, and then a maximum permittivity (36 000 at 10 kHz) at the transition temperature T-max=277 degreesC at the MPB composition. The maximum transition temperature of this system was 326 degreesC at the composition x=0.9 with the relative permittivity of 32 000 at 10 kHz. (C) 2004 American Institute of Physics.
机译:通过钴矿法合成了普通铁电体Pb(Zr1 / 2Ti1 / 2)O-3(PZT)和弛豫铁电体Pb(Ni1 / 3Nb2 / 3)O-3(PNN)之间的固溶体。研究了xPZT-(1-x)PNN的相结构和介电性能,其中x = 0.4-0.9且Zr / Ti成分固定在接近变质相界(MPB)的位置。利用这些数据,已经建立了PZT和PNN之间的铁电相图。 PNN的弛豫铁电性质逐渐向正常铁电态转变,组成为0.7PZT-0.3PNN,介电常数的特征是尖峰和分散行为的消失。 X射线衍射分析表明,在组成0.8PZT-0.2PNN的情况下,菱面体相和四方晶相共存,这是该系统中一种新的形态相边界。介电谱的检查表明,PZT-PNN在MPB组分附近表现出极高的相对介电常数。介电常数在菱面体到四方相转变温度T-RT = 195℃时显示出一个肩膀,然后在MPB组成中在转变温度T-max = 277℃时显示出最大介电常数(在10 kHz下为36000)。在组成x = 0.9下,该系统的最大转变温度为326℃,在10kHz下的相对介电常数为32 000。 (C)2004美国物理研究所。

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