首页> 外文OA文献 >Structural perspective on the anomalous weak-field piezoelectric response at the polymorphic phase boundaries of (Ba, Ca)(Ti, M)O-3 lead-free piezoelectrics (M = Zr, Sn, Hf)
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Structural perspective on the anomalous weak-field piezoelectric response at the polymorphic phase boundaries of (Ba, Ca)(Ti, M)O-3 lead-free piezoelectrics (M = Zr, Sn, Hf)

机译:(Ba,Ca)(Ti,M)O-3无铅压电(M = Zr,Sn,Hf)多态相界处异常弱场压电响应的结构透视

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摘要

Although, as part of a general phenomenon, the piezoelectric response of Ba(Ti-1 M-y(y))O-3 (M = Zr, Sn, Hf) increases in the vicinity of the orthorhombic (Amm2)-tetragonal(P4mm) and orthorhombic (Amm2)-rhombohedral (R3m) polymorphic phase boundaries, experiments in the last few years have shown that the same phase boundaries show significantly enhanced weak-field piezoproperties in the Ca-modified variants of these ferroelectric alloys, i.e., (Ba, Ca)(Ti, M)O-3. So far there is a lack of clarity with regard to the unique feature(s) which Ca modification brings about that enables this significant enhancement. Here, we examine this issue from a structural standpoint with M = Sn as a case study. We carried out a comprehensive comparative structural, ferroelectric, and piezoelectric analysis of the Amm2 phase in the immediate vicinity of the P4mm-Amm2 phase boundaries of (i) Ca-modified Ba(Ti, Sn)O-3, as per the nominal formula (1-x)BaTi0.88Sn0.12O3-(x)Ba0.7Ca0.3TiO3 and (ii) without Ca modification, i.e., Ba(Ti1-ySny) O3. We found that the spontaneous lattice strain of the Amm2 phase is noticeably smaller in the Ca-modified counterpart. Interestingly, this happens along with an improved spontaneous polarization by enhancing the covalent character of the Ti-O bond. Our study suggests that the unique role of Ca modification lies in its ability to induce these seemingly contrasting features (reduction in spontaneous lattice strain but increase in polarization).
机译:尽管作为一般现象的一部分,Ba(Ti-1 My(y))O-3(M = Zr,Sn,Hf)的压电响应在正交晶(Amm2)-四边形(P4mm)附近增加和正交晶体(Amm2)-菱面体(R3m)多晶型相界,最近几年的实验表明,相同的相界在这些铁电合金的Ca变体中显示出显着增强的弱场压电性能,即(Ba, Ca)(Ti,M)O-3。到目前为止,对于Ca修饰带来的使这种显着增强的独特特征缺乏清楚性。在这里,我们从结构的角度研究此问题,并以M = Sn作为案例研究。根据标称公式,我们对(i)Ca修饰的Ba(Ti,Sn)O-3的P4mm-Amm2相界附近的Amm2相进行了全面的比较结构,铁电和压电分析(1-x)BaTi0.88Sn0.12O3-(x)Ba0.7Ca0.3TiO3和(ii)未经Ca修饰的Ba(Ti1-ySny)O3。我们发现,在Ca修饰的对应物中,Amm2相的自发晶格应变明显较小。有趣的是,这与通过增强Ti-O键的共价特性而改善的自发极化同时发生。我们的研究表明,Ca修饰的独特作用在于其诱导这些看似相反的特征的能力(减少自发晶格应变,但增加极化)。

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