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Influence of rhombohedral stacking order in the electrical resistance of bulk and mesoscopic graphite

机译:菱面体堆积顺序对大体积和介观石墨的电阻的影响

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摘要

The electrical, in-plane resistance as a function of temperature R(T) of bulk and mesoscopic thin graphite flakes obtained from the same batch was investigated. Samples thicker than ~30 nm show metalliclike contribution in a temperature range that increases with the sample thickness, whereas a semiconductinglike behavior was observed for thinner samples. The temperature dependence of the in-plane resistance of all measured samples and several others from literature can be very well explained between 2 and 1100 K assuming three contributions in parallel: a metalliclike conducting path at the interfaces between crystalline regions, composed of two semiconducting phases, i.e., Bernal and rhombohedral stacking. From the fits of R(T) we obtain a semiconducting energy gap of 110 ± 20 meV for the rhombohedral and 38 ± 8 meV for the Bernal phase. The presence of these crystalline phases was confirmed by x-ray diffraction measurements. We review similar experimental data from literature of the last 33 years and two more theoretical models used to fit R(T).
机译:研究了从同一批次获得的块状和介观的薄石墨薄片的平面电阻与温度R(T)的关系。厚度大于〜30 nm的样品在随样品厚度增加的温度范围内表现出类似金属的作用,而对于较薄的样品则观察到类似半导体的行为。假设以下三个因素并行发生,则可以很好地解释所有测量样品以及文献中的其他几个样品的面内电阻与温度的关系:两个平行的贡献:在两个结晶相之间的晶体区域之间的界面处的类似金属的导电路径,即Bernal和菱面体堆叠。从R(T)的拟合中,我们得到菱形面体的半导体能隙为110±20 meV,伯纳尔相为38±8 meV。这些结晶相的存在通过X射线衍射测量确认。我们回顾了过去33年的文献中的类似实验数据,以及另外两个用于拟合R(T)的理论模型。

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  • 来源
    《Physical review》 |2017年第4期|045308.1-045308.11|共11页
  • 作者单位

    Division of Superconductivity and Magnetism, Institute for Experimental Physics II, University of Leipzig, D-04103 Leipzig, Germany;

    Division of Superconductivity and Magnetism, Institute for Experimental Physics II, University of Leipzig, D-04103 Leipzig, Germany;

    Division of Superconductivity and Magnetism, Institute for Experimental Physics II, University of Leipzig, D-04103 Leipzig, Germany;

    Division of Superconductivity and Magnetism, Institute for Experimental Physics II, University of Leipzig, D-04103 Leipzig, Germany;

    Division of Superconductivity and Magnetism, Institute for Experimental Physics II, University of Leipzig, D-04103 Leipzig, Germany;

    Institut fuer Mineralogie, Kristallographie und Materialwissenschaft, Fakultaet fuer Chemie und Mineralogie, Universitdt Leipzig, Scharnhorststrasse 20, D-04275 Leipzig, Germany;

    Institut fuer Mineralogie, Kristallographie und Materialwissenschaft, Fakultaet fuer Chemie und Mineralogie, Universitdt Leipzig, Scharnhorststrasse 20, D-04275 Leipzig, Germany;

    Institute for Medicine Physics and Biophysics, University of Leipzig, D-04107 Leipzig, Germany;

    Institute for Medicine Physics and Biophysics, University of Leipzig, D-04107 Leipzig, Germany;

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