超声换能器用压电PZN-PT 91/9和PMN-PT 66/34单晶的生长和表征

J. Santailler, B. Ferrand, Dragan Damjanovic, M. Couchaud, P. Dusserre, M. Budimir, S. Mibord, T. Abad
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引用次数: 0

摘要

如今,足够尺寸的高晶体质量和高晶体生长率似乎是铁电材料广泛推广和应用的关键。因此,本文研究了PZN-PT固溶体化合物如(1-x)(PbZn/sub 1/3/Nb/sub 2/3/O/sub 3/)-xPbTiO/sub 3/和PMN-PT化合物如(1-y)(PbMg/sub 1/3/Nb/sub 2/3/O/sub 3/)-yPbTiO/sub 3/的生长。这两种弛豫铁电单晶在嗜形相边界(MPB)转变附近获得了良好的性能,PZN-PT在x=0.09和PMN-PT在y=0.34附近发生转变。复合单晶相转变结合适当的外加电场,在pseudo /sub /方向取向;赋予这些单晶一些有趣的压电性质。本文介绍了PZN-PT的垂直梯度冷冻溶液生长方法(VGF-SG)和PMN-PT的伪Kyropoulos生长方法的一些晶体生长结果。所得的单晶,PZN-PT高达120 g, PMN-PT高达160 g,然后分析其组成和结构。PMN-PT和PZN-PT钙钛矿晶体均为菱形(@RT),具有良好的整体均匀性。样品表现出铁电行为,极化处理后,PZN-PT在居里温度(Tc /spl sim/174/spl度/C @ 1kHz)附近的介电常数高达48000,PMN-PT (Tc /spl sim/ 142/spl度/C @ 100 Hz)的介电常数为74000。压电系数d/sub 33/给出PZN-PT高达/spl sim/2200 pC/N(@RT 9 kV/cm)和PMN-PT 1700 pC/N(@RT)的值。机电耦合系数k/sub / 33的测量值高达94%。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Growth and characterisation of piezoelectric PZN-PT 91/9 and PMN-PT 66/34 single crystals for ultrasonic transducers
Today, high crystal quality in sufficient size with high crystal growth yield appears to be a key point for a wide dissemination and use in ferroelectrics applications. So, this paper is related to the growth of PZN-PT solid solution compound like (1-x)(PbZn/sub 1/3/Nb/sub 2/3/O/sub 3/)-xPbTiO/sub 3/ and PMN-PT compound like (1-y)(PbMg/sub 1/3/Nb/sub 2/3/O/sub 3/)-yPbTiO/sub 3/. For these two relaxor ferroelectric single crystals promising properties are obtained near the Morphotropic Phase Boundary (MPB) transition which occurred at values closed to x=0.09 for PZN-PT and y=0.34 for PMN-PT. The complex unit cell phase transition combined with an adequate applied electric field, oriented in the pseudo <001>/sub c/ direction; confer to these single crystals some interesting piezoelectric properties. We present some crystal growth results obtained by the Vertical Gradient Freeze-Solution Growth method (VGF-SG) for PZN-PT and by a pseudo Kyropoulos method developed for PMN-PT. The obtained single crystals, up to 120 g for PZN-PT and 160 g for PMN-PT are then analysed in term of composition and structure. Both PMN-PT and PZN-PT perovskite crystals are rhombohedral (@RT), they show a good global homogeneity. Samples demonstrate ferroelectric behaviour, and after polarisation process, dielectric constants up to 48000 near the Curie temperature (Tc /spl sim/174/spl deg/C @ 1kHz) are obtained for PZN-PT and respectively 74000 for PMN-PT (Tc /spl sim/ 142/spl deg/C @ 100 Hz). The piezoelectric coefficient d/sub 33/ gives values up to /spl sim/2200 pC/N (@RT 9 kV/cm) for PZN-PT and 1700 pC/N(@RT) for PMN-PT. A value up to 94% is measured for the electromechanical coupling coefficient k/sub 33/.
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