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Tunable strain effect and ferroelectric field effect on the electronic transport properties of La_(0.5)Sr_(0.5)CoO_3 thin films

机译:可调应变效应和铁电场效应对La_(0.5)Sr_(0.5)CoO_3薄膜的电子输运性能的影响

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摘要

Tensiled La_(0.5)Sr_(0.5)CoO_3 (LSCO) thin films were epitaxially grown on piezoelectric 0.67Pb (Mg_(1/3)Nb_(2/3)O_3-0.33PbTiO_3 (PMN-PT) single-crystal substrates. Due to the epitaxial nature of the interface, the lattice strain induced by ferroelectric poling or the converse piezoelectric effect in the PMN-PT substrate is effectively transferred to the LSCO film and thus reduces the tensile strain of the film, giving rise to a decrease in the resistivity of the LSCO film. We discuss these strain effects within the framework of the spin state transition of Co~(3+) ions and modification of the electronic bandwidth that is relevant to the induced strain. By simultaneously measuring the strain and the resistivity, quantitative relationship between the resistivity and the strain was established for the LSCO film. Both theoretical calculation and experimental results demonstrate that the ferroelectric field effect at room temperature in the LSCO/PMN-PT field-effect transistor is minor and could be neglected. Nevertheless, with decreasing temperature, the ferroelectric field effect competes with the strain effect and plays a more and more important role in influencing the electronic transport properties of the LSCO film, which we interpreted as due to the localization of charge carriers at low temperature.
机译:在压电0.67Pb(Mg_(1/3)Nb_(2/3)O_3-0.33PbTiO_3(PMN-PT)单晶衬底上外延生长Tensiled La_(0.5)Sr_(0.5)CoO_3(LSCO)薄膜。由于界面的外延特性,铁电极化引起的晶格应变或PMN-PT基板中的逆压电效应会有效地转移到LSCO膜上,从而降低膜的拉伸应变,从而导致膜厚的减小。 LSCO薄膜的电阻率,我们在Co〜(3+)离子的自旋态跃迁和与感应应变相关的电子带宽的改变的框架内讨论了这些应变效应,同时测量应变和电阻率,建立了LSCO薄膜电阻率与应变的定量关系,理论计算和实验结果均表明LSCO / PMN-PT场效应晶体管在室温下的铁电场效应较小,且可以忽略。然而,随着温度的降低,铁电场效应与应变效应竞争,并且在影响LSCO薄膜的电子传输性能中起着越来越重要的作用,我们将其解释为由于载流子在低温下的局部化。

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  • 来源
    《Journal of Applied Physics》 |2012年第10期|p.103702.1-103702.7|共7页
  • 作者单位

    State Key Laboratory of High Performance Ceramics and Superfine Microstructure, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, China,Graduate School of Chinese Academy of Sciences, Beijing 100039, China;

    State Key Laboratory of High Performance Ceramics and Superfine Microstructure, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, China;

    State Key Laboratory of High Performance Ceramics and Superfine Microstructure, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, China;

    State Key Laboratory of High Performance Ceramics and Superfine Microstructure, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, China;

    Department of Applied Physics and Materials Research Center, The Hong Kong Polytechnic University, Hong Kong, China;

    State Key Laboratory of High Performance Ceramics and Superfine Microstructure, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, China;

    Department of Applied Physics and Materials Research Center, The Hong Kong Polytechnic University, Hong Kong, China;

    State Key Laboratory of High Performance Ceramics and Superfine Microstructure, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, China,Department of Applied Physics and Materials Research Center, The Hong Kong Polytechnic University, Hong Kong, China;

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