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Phase coherent transport in graphene nanoribbons and graphene nanoribbon arraysud

机译:石墨烯纳米带和石墨烯纳米带阵列中的相干相干传输 ud

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摘要

We have experimentally investigated quantum interference corrections to the conductivity of graphene nanoribbons at temperatures down to 20 mK studying both weak localization (WL) and universal conductance fluctuations (UCFs). Since in individual nanoribbons at milli-Kelvin temperatures the UCFs strongly mask the weak localization feature we employ both gate averaging and ensemble averaging to suppress the UCFs. This allows us to extract the phase coherence length from both WL and UCF at all temperatures. Above 1 K the phase coherence length is suppressed due to Nyquist scattering, whereas at low temperatures we observe a saturation of the phase coherence length at a few hundred nanometers, which exceeds the ribbon width, but stays below values typically found in bulk graphene. To better describe the experiments at elevated temperatures, we extend the formula for one-dimensional (1D) weak localization in graphene, which was derived in the limit of strong intervalley scattering, to include all elastic scattering rates.
机译:我们已通过实验研究了弱局部化(WL)和通用电导涨落(UCF),研究了石墨烯纳米带在低至20 mK的温度下的电导率量子校正。由于在毫开氏温度下的单个纳米带中,UCF强烈地掩盖了弱的局部化特征,因此我们采用门平均和集合平均来抑制UCF。这使我们能够在所有温度下从WL和UCF提取相干长度。在1 K以上,由于奈奎斯特散射,相干长度受到抑制,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,但仍低于通常在体石墨烯中发现的值。为了更好地描述在高温下的实验,我们扩展了石墨烯中的一维(1D)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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