首页> 外文期刊>Journal of Applied Physics >Comparison of the structural properties of Zn-face and O-face single crystal homoepitaxial ZnO epilayers grown by RF-magnetron sputtering
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Comparison of the structural properties of Zn-face and O-face single crystal homoepitaxial ZnO epilayers grown by RF-magnetron sputtering

机译:射频磁控溅射生长Zn面和O面单晶同质外延ZnO外延层的结构特性比较

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摘要

Homoepitaxial ZnO growth is demonstrated from conventional RF-sputtering at 400℃ on both Zn and O polar faces of hydrothermally grown ZnO substrates. A minimum yield for the Rutherford backscattering and channeling spectrum, X_(min), equal to ~3% and ~12% and a full width at half maximum of the 00.2 diffraction peak rocking curve of (70 ± 10) arc sec and (1400 ± 100) arc sec have been found for samples grown on the Zn and O face, respectively. The structural characteristics of the film deposited on the Zn face are comparable with those of epilayers grown by more complex techniques like molecular beam epitaxy. In contrast, the film simultaneously deposited on the O-face exhibits an inferior crystalline structure ~0.7% strained in the c-direction and a higher atomic number contrast compared with the substrate, as revealed by high angle annular dark field imaging measurements. These differences between the Zn- and O-face films are discussed in detail and associated with the different growth mechanisms prevailing on the two surfaces.
机译:通过在400℃下对水热生长的ZnO衬底的Zn和O极性表面进行常规的RF溅射可以证明同质外延ZnO的生长。卢瑟福背向散射和通道光谱的最小屈服X_(min)等于〜3%和〜12%,并且00.2衍射峰摇摆曲线的半峰全宽为(70±10)弧秒和(1400)已发现分别在Zn和O面上生长的样品的±100)弧秒。沉积在Zn面上的薄膜的结构特征与通过更复杂的技术(如分子束外延)生长的外延层的结构特征相当。相反,同时沉积在O面上的薄膜与衬底相比,在c方向上应变的晶体结构差〜0.7%,并且原子序数对比度更高,这是通过高角度环形暗场成像测量得出的。详细讨论了Zn和O面膜之间的这些差异,并将它们与两个表面上普遍存在的不同生长机制相关联。

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  • 来源
    《Journal of Applied Physics》 |2017年第1期|015304.1-015304.8|共8页
  • 作者单位

    Department of Physicsl Center for Material Science and Nanotechnology, University of Oslo, P.O. Box 1048, Blindern, N-0316 Oslo, Norway,Institute of Physics, Polish Academy of Sciences, Al. Lotnikow 32146, 02-668 Warsaw, Poland;

    Department of Physicsl Center for Material Science and Nanotechnology, University of Oslo, P.O. Box 1048, Blindern, N-0316 Oslo, Norway;

    Institute of Physics, Polish Academy of Sciences, Al. Lotnikow 32146, 02-668 Warsaw, Poland;

    Department of Physicsl Center for Material Science and Nanotechnology, University of Oslo, P.O. Box 1048, Blindern, N-0316 Oslo, Norway;

    National Centre for Nuclear Research, A. Soltana 7, 05-400 Otwock-Swierk, Poland;

    Department of Physicsl Center for Material Science and Nanotechnology, University of Oslo, P.O. Box 1048, Blindern, N-0316 Oslo, Norway;

    Department of Physicsl Center for Material Science and Nanotechnology, University of Oslo, P.O. Box 1048, Blindern, N-0316 Oslo, Norway;

    Department of Physicsl Center for Material Science and Nanotechnology, University of Oslo, P.O. Box 1048, Blindern, N-0316 Oslo, Norway;

    Department of Electronic Materials Engineering, Research School of Physics and Engineering and Centre for Advanced Microscopy, The Australian National University, Canberra, Australian Capital Territory 2601, Australia;

    Department of Electronic Materials Engineering, Research School of Physics and Engineering and Centre for Advanced Microscopy, The Australian National University, Canberra, Australian Capital Territory 2601, Australia;

    Department of Physicsl Center for Material Science and Nanotechnology, University of Oslo, P.O. Box 1048, Blindern, N-0316 Oslo, Norway;

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