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首页> 外文期刊>Angewandte Chemie >Polarization Rotation in the Monoclinic Perovskite BiCo_(1-x)Fe_O3
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Polarization Rotation in the Monoclinic Perovskite BiCo_(1-x)Fe_O3

机译:单斜钙钛矿BiCo_(1-x)Fe_O3的极化旋转

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A piezoelectric ceramic, Pb(Ti_(1-x)Zr_x)O3 (PZT), is widely used for various applications, such as transducers and sensors. PZT shows a maximum piezoelectric effect with a composition of about x = 0.5, the boundary separating the tetragonal PAmm (Ti-rich) and the rhombohedral Rim (Zr-rich) phases in the phase diagram. This boundary is known as a morphotropic phase boundary (MPB).Investigation of the structural evolution at the MPB is indispensable for understanding the origin of the enhanced piezoelectric property in PZT. In 2000, Noheda reported the presence of a monoclinic phase at x = 0.50 and 0.52 below 200 and 250 K, respectively, on the basis of powder synchrotron X-ray diffraction (SXRD) studies. The monoclinic phase had a √2a x √2a x a unit cell, where a was the cubic perovskite lattice parameter and the space group was Cm. This finding explains the mechanism of the piezoelectric enhancement as follows. The lack of a symmetry axis in the monoclinic structure allows the rotation of the ferroelectric polarization vector between the polar axes of the tetragonal and rhombohedral phases. This polarization rotation is induced by applying an electric field, leading to the enhancement of the piezoelectric constant.Although the large piezoelectric response of PZT is successfully explained, the presence of a monoclinic phase in PZT as a distinct phase is controversial. The insufficient difference in the pseudo cubic unit cell parameters of tetragonal, rhombohedral, and monoclinic phases inhibits the structural analysis based on diffraction studies. The cla ratio of tetragonal (P4mm) PbTi_(0.48)Zr_(0.52)O3 at 325 K is 1.01, which is quite close to unity, and the a of rhombohedral (Rim) PbTi_(0.40)Zr_(0.60)O3 at 295 K is 90.45°, that is, almost orthogonal. The monoclinic phase has an intermediate structure between the tetragonal and the rhombohedral phases. These three phases are thus so close to cubic that their diffraction peaks overlap extremely.
机译:压电陶瓷Pb(Ti_(1-x)Zr_x)O3(PZT)被广泛用于各种应用,例如换能器和传感器。 PZT表现出最大的压电效应,其成分约为x = 0.5,在相图中,边界将四方PAmm(富Ti)相和菱面Rim(富Zr)相隔开。该边界被称为同相相边界(MPB)。为了了解PZT中增强的压电特性的起源,研究MPB处的结构演化是必不可少的。 2000年,根据粉末同步辐射X射线衍射(SXRD)研究,Noheda报道在200 K和250 K以下x分别存在x = 0.50和0.52的单斜晶相。单斜晶相的晶胞为√2ax√2ax,其中a为立方钙钛矿晶格参数,空间群为Cm。该发现如下解释了压电增强的机理。单斜晶结构中不存在对称轴,使得铁电极化矢量在四方相和菱形相的极轴之间旋转。这种极化旋转是通过施加电场引起的,从而导致压电常数的提高。尽管已成功地解释了PZT的大压电响应,但在PZT中存在单斜相作为独特相存在争议。四方,菱面体和单斜晶相的拟立方晶胞参数之间的差异不足,会抑制基于衍射研究的结构分析。在325 K时四方(P4mm)PbTi_(0.48)Zr_(0.52)O3的cla比为1.01,非常接近于1;在295 K时菱形(Rim)PbTi_(0.40)Zr_(0.60)O3的cla值是90.45°,即几乎正交。单斜晶相在四方相和菱面体相之间具有中间结构。因此,这三个相非常接近立方,以致它们的衍射峰极为重叠。

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