首页> 外文期刊>Journal of Applied Physics >Electrical properties of K_(0.5)Na_(0.5)NbO_3 thin films grown on Nb:SrTiO_3 single-crystalline substrates with different crystallographic orientations
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Electrical properties of K_(0.5)Na_(0.5)NbO_3 thin films grown on Nb:SrTiO_3 single-crystalline substrates with different crystallographic orientations

机译:在不同晶体取向的Nb:SrTiO_3单晶衬底上生长的K_(0.5)Na_(0.5)NbO_3薄膜的电性能

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摘要

To attain a deep understanding of ferroelectric and piezoelectric characteristics of K_(0.5)Na_(0.5)NbO_3 as a promising lead-free compound, the ferroelectric and piezoelectric responses of its epitaxially grown films with three primary orientations of [001], [110], and [111] were investigated with an emphasis on the influence of crystallographic orientation. The films were prepared by sol-gel processing using Nb-doped SrTiO_3 single-crystalline substrates with various cutting directions. A peak remnant polarization value (P_r) of 17.3μC/cm~2 was obtained along the [110] direction due to the coincidence between the spontaneous polarization and the film orientation, which is significantly higher than 10.5 μC/cm~2 in [11 l]-oriented and 10.1 μC/cm~2 in [001]-oriented ones. However, a better piezoelectric response was achieved in the [001]-oriented films with an average local effective piezoelectric coefficient (d_33) of 50.5 pm/V, as compared with 45.1 pm/V and 39.7 pm/V in [110]- and [111]-oriented films, respectively.
机译:为了深入了解K_(0.5)Na_(0.5)NbO_3作为有前途的无铅化合物的铁电和压电特性,其外延生长膜的三个主要方向[001],[110]的铁电和压电响应,[111]的研究重点是晶体学取向的影响。通过使用Nb掺杂的SrTiO_3单晶衬底以各种切割方向通过溶胶-凝胶工艺制备薄膜。由于自发极化和薄膜取向的重合,沿[110]方向获得的残余极化峰峰值(P_r)为17.3μC/ cm〜2,远高于[11]中的10.5μC/ cm〜2。面向[l]方向,在[001]方向中为10.1μC/ cm〜2。但是,在[001]取向的薄膜中,平均局部有效压电系数(d_33)为50.5 pm / V,与[110]-薄膜中的45.1 pm / V和39.7 pm / V相比,压电响应更好。 [111]面向电影。

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  • 来源
    《Journal of Applied Physics》 |2013年第2期|024101.1-024101.5|共5页
  • 作者单位

    Department of Materials Science and Engineering, State Key Laboratory of New Ceramics and Fine Processing, Tsinghua University, 100084 Beijing, People's Republic of China;

    Department of Materials Science and Engineering, State Key Laboratory of New Ceramics and Fine Processing, Tsinghua University, 100084 Beijing, People's Republic of China;

    Department of Materials Science and Engineering, State Key Laboratory of New Ceramics and Fine Processing, Tsinghua University, 100084 Beijing, People's Republic of China;

    Department of Materials Science and Engineering, State Key Laboratory of New Ceramics and Fine Processing, Tsinghua University, 100084 Beijing, People's Republic of China;

    Department of Materials Science and Engineering, State Key Laboratory of New Ceramics and Fine Processing, Tsinghua University, 100084 Beijing, People's Republic of China;

    Department of Materials Science and Engineering, State Key Laboratory of New Ceramics and Fine Processing, Tsinghua University, 100084 Beijing, People's Republic of China;

    Department of Materials Science and Engineering, State Key Laboratory of New Ceramics and Fine Processing, Tsinghua University, 100084 Beijing, People's Republic of China;

    Department of Mechanical Engineering and Materials Science, University of Pittsburgh, Pittsburgh, Pennsylvania 15261, USA;

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