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Dirac point resonances due to atoms and molecules adsorbed on graphene and transport gaps and conductance quantization in graphene nanoribbons with eovalently bonded adsorbates

机译:吸附在石墨烯上的原子和分子的狄拉克点共振,以及具有等价键合吸附物的石墨烯纳米带中的传输间隙和电导量化

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We present a tight-binding theory of the Dirac point resonances due to adsorbed atoms and molecules on an infinite two-dimensional graphene sheet based on the standard tight-binding model of the graphene jr-band electronic structure and the extended Hiickel model of the adsorbate and nearby graphene carbon atoms. The relaxed atomic geometries of the adsorbates and graphene are calculated using density functional theory. Our model includes the effects of local rehybridization of the graphene from the sp2 to sp3 electronic structures that occurs when adsorbed atoms or molecules bond eovalently to the graphene. Unlike in previous tight-binding models of Dirac point resonances, adsorbed species with multiple extended molecular orbitals and bonding to more than one graphene carbon atom are treated. More accurate and more general analytic expressions for the Green's function matrix elements that enter the T-matrix theory of Dirac point resonances than have been available previously are obtained. We study H, F, OH, and O adsorbates on graphene and for each we find a strong scattering resonance (two resonances for O) near the Dirac point of graphene, by far the strongest and closest to the Dirac point being the resonance for H. We extract a minimal set of tight-binding parameters that can be used to model resonant electron scattering and electron transport in graphene and graphene nanostructures with adsorbed H, F, OH, and O accurately and efficiently. We also compare our results for the properties of Dirac point resonances due to adsorbates on graphene with those obtained by others using density-functional-theory-based electronic structure calculations and discuss their relative merits. We then present calculations of electronic quantum transport in graphene nanoribbons with these adsorbed species. Our transport calculations capture the physics of the scattering resonances that are induced in the graphene ribbons near the Dirac point by the presence of the adsorbates. We find that the Dirac point resonances play a dominant role in quantum transport in ribbons with adsorbates: Even at low adsorbate concentrations the conductance of the ribbon is strongly suppressed and a transport gap develops for electron Fermi energies near the resonance. The transport gap is centered very near the Dirac point energy for H, below it for F and OH, and above it for O. We find conduction in ribbons with adsorbed H atoms to be very similar to that in ribbons with equal concentrations of carbon atom vacancies. We predict ribbons with adsorbed H, F, OH, and O, under appropriate conditions, to exhibit quantized conductance steps of equal height, similar to those that have been observed by Lin et al. [Phys. Rev. B 78, 161409(R) (2008)] at moderately low temperatures, even for ribbons with conductances a few orders of magnitude smaller than2e~2/h.
机译:我们基于石墨烯jr带电子结构的标准紧密结合模型和被吸附物的扩展Hiickel模型,提出了无限二维石墨烯片材上由于吸附的原子和分子而引起的狄拉克点共振的紧密结合理论和附近的石墨烯碳原子。使用密度泛函理论计算吸附物和石墨烯的弛豫原子几何形状。我们的模型包括当吸附的原子或分子与石墨烯等价键合时发生的石墨烯从sp2到sp3电子结构的局部再杂交的影响。与以前的狄拉克点共振紧密结合模型不同,具有多个扩展分子轨道并与一个以上石墨烯碳原子键合的吸附物质得到了处理。获得了格林函数矩阵元素的更准确,更通用的解析表达式,这些表达式进入了狄拉克点共振的T矩阵理论,比以前可获得的表达式更精确。我们研究了石墨烯上的H,F,OH和O吸附物,并在石墨烯的狄拉克点附近发现了强散射散射(O的两个共振),到目前为止,最强且最接近Dirac点的是H的共振我们提取了最小限度的紧密结合参数集,这些参数可用于模拟准确有效地吸附H,F,OH和O的石墨烯和石墨烯纳米结构中的共振电子散射和电子传输。我们还比较了我们在石墨烯上吸附物与其他人使用基于密度泛函理论的电子结构计算获得的狄拉克点共振性质的结果,并讨论了它们的相对优点。然后,我们介绍了具有这些吸附物种的石墨烯纳米带中电子量子传输的计算。我们的传输计算记录了由于吸附物的存在在Dirac点附近的石墨烯碳带中引起的散射共振的物理现象。我们发现,狄拉克点共振在带被吸附物的碳带中的量子传输中起主要作用:即使在低吸附物浓度下,碳带的电导也被强烈抑制,并且在共振附近电子的费米能量产生了传输间隙。传输间隙的中心非常接近H的狄拉克点能量,F和OH低于该能量,O高于该能量。我们发现,吸附有H原子的碳带的导电性与碳原子浓度相同的碳带的导电性非常相似。空缺。我们预测在适当的条件下,吸附有H,F,OH和O的碳带将显示出相等高度的量化电导阶跃,类似于Lin等人所观察到的。 [物理Rev. B 78,161409(R)(2008)]在中等低温下,即使对于电导小于2e〜2 / h几个数量级的碳带也是如此。

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