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

机译:菱形堆叠顺序在散装和介读石墨电阻中的影响

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摘要

The electrical, in-plane resistance as a function of temperatureR(T ) of bulk and mesoscopic thin graphite flakesobtained from the same batch was investigated. Samples thicker than ~30 nm show metalliclike contribution in atemperature range that increases with the sample thickness, whereas a semiconductinglike behavior was observedfor thinner samples. The temperature dependence of the in-plane resistance of all measured samples and severalothers 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 semiconductingphases, i.e., Bernal and rhombohedral stacking. From the fits of R(T ) we obtain a semiconducting energy gapof 110 ± 20 meV for the rhombohedral and 38 ± 8 meV for the Bernal phase. The presence of these crystallinephases was confirmed by x-ray diffraction measurements.We review similar experimental data from literature ofthe last 33 years and two more theoretical models used to fit R(T ).
机译:作为散装和介型薄石墨薄片的温度(t)的功能的电气,面内阻研究了从相同的批次获得。样品比〜30 nm厚,显示了金属般的贡献随着样品厚度增加的温度范围,而观察到半导体样行为用于更薄的样品。所有测量样本的面内阻的温度依赖性和几个来自文学的其他人可以在2到1100 k之间进行很好的解释,假设三个贡献并行:在晶体区之间的界面处的金属状导电路径,由两个半导体组成阶段,即伯纳尔和菱形堆叠。从R(t)的配合来看,我们获得半导体能量隙为菱面向110±20米,为伯纳阶段的38±8米。这些结晶的存在通过X射线衍射测量确认阶段。我们从文献中审查了类似的实验数据过去33年和两个用于适合R(T)的理论模型。

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  • 来源
    《Physical Review. B, Condensed Matter》 |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 Universitaet Leipzig Scharnhorststrasse 20 D-04275 Leipzig Germany;

    Institut fuer Mineralogie Kristallographie und Materialwissenschaft Fakultaet fuer Chemie und Mineralogie Universitaet 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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