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Phase Coherent Transport in Graphene Nanoribbons and Graphene Nanoribbon Arrays

机译:石墨烯纳米带和石墨烯纳米带中的相位相干输运   数组

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摘要

We have experimentally investigated quantum interference corrections to theconductivity of graphene nanoribbons at temperatures down to 20 mK studyingboth weak localization (WL) and universal conductance fluctuations (UCF). Sincein individual nanoribbons at millikelvin temperatures the UCFs strongly maskthe weak localization feature we employ both gate averaging and ensembleaveraging to suppress the UCFs. This allows us to extract the phase coherencelength from both WL and UCF at all temperatures. Above 1 K, the phase coherencelength is suppressed due to Nyquist scattering whereas at low temperatures weobserve a saturation of the phase coherence length at a few hundred nanometers,which exceeds the ribbon width, but stays below values typically found in bulkgraphene. To better describe the experiments at elevated temperatures, weextend the formula for 1D weak localization in graphene, which was derived inthe limit of strong intervalley scattering, to include all elastic scatteringrates.
机译:我们通过弱定位(WL)和通用电导涨落(UCF)研究了在低至20 mK的温度下对石墨烯纳米带导电性的量子干涉校正。由于在毫微卡尔文温下的单个纳米带中,UCF强烈掩盖了弱的定位功能,因此我们采用门平均和整体平均来抑制UCF。这使我们能够在所有温度下从WL和UCF提取相位相干长度。高于1 K时,由于Nyquist散射而抑制了相干长度,而在低温下,我们观察到相干长度在几百纳米处达到饱和,超过了带的宽度,但仍低于体石墨烯中的典型值。为了更好地描述高温下的实验,我们扩展了石墨烯中一维弱局部化的公式,该公式是在强间隔胶束散射的限制下得出的,以包括所有弹性散射率。

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