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首页> 外文期刊>Journal of Applied Physics >Pyroelectric properties of (1-x)Pb(Mg1/3Nb2/3)O-3-xPbTiO(3) and (1-x)Pb(Zn1/3Nb2/3)O-3-xPbTiO(3) single crystals measured using a dynamic method
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Pyroelectric properties of (1-x)Pb(Mg1/3Nb2/3)O-3-xPbTiO(3) and (1-x)Pb(Zn1/3Nb2/3)O-3-xPbTiO(3) single crystals measured using a dynamic method

机译:(1-x)Pb(Mg1 / 3Nb2 / 3)O-3-xPbTiO(3)和(1-x)Pb(Zn1 / 3Nb2 / 3)O-3-xPbTiO(3)单晶的热电性能动态方法

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摘要

The pyroelectric coefficients of 0.72Pb(Mg1/3Nb2/3)O-3-0.28PbTiO(3) (PMN-28PT), 0.67Pb(Mg1/3Nb2/3)O-3-0.33PbTiO(3) (PMN-33PT), and 0.92 Pb(Zn1/3Nb2/3)O-3-0.08PbTiO(3) (PZN-8PT) single crystals, oriented and poled along three different crystallographic directions, [001](C), [011](C), and [111](C), have been measured using a dynamic method. The suffix C indicates reference to the prototypic cubic coordinate system. Large coefficients of up to 1070 mu C m(-2) K-1 have been observed for the [111](C) oriented, rhombohedral PMN-28PT and PMN-33PT samples, where the measurement direction corresponds to the polar axis of the crystal. For each composition and orientation two different poling procedures are compared, a commonly used field cooling method and a low temperature poling protocol. It was found that in otherwise pseudoorthorhombic samples of PZN-8PT, a room temperature rhombohedral phase could be stabilized by application of a field along the [111](C) direction while heating from -70degreesC. (C) 2004 American Institute of Physics.
机译:0.72Pb(Mg1 / 3Nb2 / 3)O-3-0.28PbTiO(3)(PMN-28PT),0.67Pb(Mg1 / 3Nb2 / 3)O-3-0.33PbTiO(3)(PMN-33PT)的热电系数)和0.92 Pb(Zn1 / 3Nb2 / 3)O-3-0.08PbTiO(3)(PZN-8PT)单晶,它们沿着三个不同的晶体学方向[001](C)和[011](C )和[111](C),已使用动态方法进行了测量。后缀C表示参考原型三次坐标系。对于[111](C)取向的菱面体PMN-28PT和PMN-33PT样品,观察到高达1070μC m(-2)K-1的大系数,其中测量方向对应于样品的极轴水晶。对于每种成分和取向,都比较了两种不同的极化程序,一种常用的现场冷却方法和一种低温极化方案。已经发现,在其他方式的PZN-8PT准斜方晶样品中,通过沿[111](C)方向施加磁场,同时从-70℃加热,可以稳定室温的菱面体相。 (C)2004美国物理研究所。

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