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Control of tensile stress on inducing formation and tunability of (100) oriented Pb_xSr_(1-x)TiO_3 thin films

机译:张应力对诱导(100)取向Pb_xSr_(1-x)TiO_3薄膜的形成和可调性的控制

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摘要

(100) Oriented Pb_xSr_(1-x)TiO_3 (PSTO) thin films are prepared on indium tin oxide (ITO)/glass substrates by sol-gel technique while inserting doped PbTiO_3 (PTO)-inducing layer in between. The effect of tensile stress in PSTO on tunability and (100) orientation of the thin films was investigated using X-ray diffraction, scanning electron microscopy, transmission electron microscope, and atomic force microscope, respectively. Results show that PSTO thin film deposited on doped PTO has (100) oriented structure while it is randomly oriented when deposited directly on the ITO/glass substrate. Lattice mismatch between PSTO and PTO appears, in which the in-plane lattice constant c is 0.3922-0.3924 nm in the former and 4.02-4.07 nm in the latter, respectively, contributing tensile stress in the PSTO due to different lattice constants between them. The stress in the PSTO thin film is 3.04, 3.15, 3.59 and 4.47 GPa when the doped PTOs are Fe-PTO, Tb-PTO, Co-PTO and Zn-PTO, respectively. The orientation degrees of PSTO thin films are from 89.63, 90.31, 91.92 to 93.29 % with increasing stress of PSTO on Fe-PTO, Tb-PTO, Co-PTO and Zn-PTO, respectively. Tunabilities of the well-oriented PSTO thin films increase in ascending order of 63 < 65 < 69 < 73 % when induced by oriented PTO layers of Fe-PTO, Tb-PTO, Co-PTO and Zn-PTO, respectively, which is in accordance with the degree of (100) orientation appearing in the thin films. The high tunability appears in the PSTO thin film while high (100) orientation is derived from the tensile stress. It is much higher than that of randomly oriented PSTO thin film.
机译:(100)通过溶胶-凝胶技术在铟锡氧化物(ITO)/玻璃基板上插入定向的Pb_xSr_(1-x)TiO_3(PSTO)薄膜,同时在其间插入掺杂的PbTiO_3(PTO)诱导层。分别使用X射线衍射,扫描电子显微镜,透射电子显微镜和原子力显微镜研究了PSTO中拉应力对薄膜的可调谐性和(100)取向的影响。结果表明,沉积在掺杂PTO上的PSTO薄膜具有(100)取向的结构,而直接沉积在ITO /玻璃基板上时它是随机取向的。 PSTO和PTO之间出现晶格失配,其中前者的面内晶格常数c为0.3922-0.3924 nm,后者的面内晶格常数c为4.02-4.07 nm,这归因于PSTO和PTO的面内晶格常数不同。当掺杂的PTO分别为Fe-PTO,Tb-PTO,Co-PTO和Zn-PTO时,PSTO薄膜中的应力为3.04、3.15、3.59和4.47 GPa。随着PSTO在Fe-PTO,Tb-PTO,Co-PTO和Zn-PTO上的应力增加,PSTO薄膜的取向度分别为89.63%,90.31、91.92至93.29%。当分别由Fe-PTO,Tb-PTO,Co-PTO和Zn-PTO的取向PTO层诱导时,取向良好的PSTO薄膜的可调谐性按63 <65 <69 <73%的升序增加。根据在薄膜中出现的(100)取向的程度。高可调性出现在PSTO薄膜中,而高(100)取向源自拉伸应力。它远高于随机取向的PSTO薄膜。

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  • 来源
    《Applied Physics》 |2014年第3期|1171-1177|共7页
  • 作者单位

    State Key Laboratory of Silicon Materials, Department of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, China;

    State Key Laboratory of Silicon Materials, Department of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, China;

    State Key Laboratory of Silicon Materials, Department of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, China;

    State Key Laboratory of Silicon Materials, Department of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, China;

    State Key Laboratory of Silicon Materials, Department of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, China;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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  • 正文语种 eng
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