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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 covalently bonded adsorbates

机译:由于吸附在石墨烯上的原子和分子,狄拉克点共振   石墨烯纳米带中的传输间隙和电导量子化   共价键合的吸附物

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摘要

We present a tight binding theory of the Dirac point resonances due toadsorbed atoms and molecules on an infinite 2D graphene sheet based on thestandard tight binding model of the graphene p-band electronic structure andthe extended Huckel model of the adsorbate and nearby graphene carbon atoms.The relaxed atomic geometries of the adsorbates and graphene are calculatedusing density functional theory. Our model includes the effects of the localrehybridization of the graphene from the sp^2 to sp^3 electronic structure thatoccurs when adsorbed atoms or molecules bond covalently to the graphene. Unlikein previous tight-binding models of Dirac point resonances, adsorbed specieswith multiple extended molecular orbitals and bonding to more than one graphenecarbon atom are treated. More accurate and more general analytic expressionsfor the Green's function matrix elements that enter the T-matrix theory ofDirac point resonances than have been available previously are obtained. Westudy H, F, OH and O adsorbates on graphene and for each we find a strongscattering 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 modelresonant electron scattering and electron transport in graphene and graphenenanostructures with adsorbed H, F, OH and O accurately and efficiently. We alsocompare our results for the properties of Dirac point resonances due toadsorbates on graphene with those obtained by others using density functionaltheory-based electronic structure calculations, and discuss their relativemerits. We then present calculations of electronic quantum transport ingraphene nanoribbons with these adsorbed species...
机译:我们基于石墨烯p带电子结构的标准紧密结合模型以及被吸附物和附近石墨烯碳原子的扩展Huckel模型,提出了无限二维石墨烯片材上吸附的原子和分子引起的狄拉克点共振的紧密结合理论。利用密度泛函理论计算了被吸附物和石墨烯的弛豫原子几何。我们的模型包括石墨烯从sp ^ 2到sp ^ 3电子结构的局部再杂交的影响,当吸附的原子或分子与石墨烯共价键合时,sp ^ 3电子结构发生。与以前的狄拉克点共振的紧密结合模型不同,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种得到了处理。对于格林函数矩阵元素,它们进入狄拉克点共振的T矩阵理论比以前已经获得了更准确,更通用的解析表达式。 Westudy H,F,OH和O吸附在石墨烯上,在石墨烯的狄拉克点附近,每一个我们都发现一个强散射共振(O的两个共振),到目前为止,最强和最接近Dirac点的是H的共振。最小的紧密结合参数集,可用于精确高效地模拟石墨烯和石墨烯结构中的共振电子散射和电子传输,并吸附有H,F,OH和O。我们还比较了由于石墨烯上的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的性质而得出的结果,并讨论了它们的相对优点。然后,我们用这些吸附的物种给出电子量子传输石墨烯纳米带的计算...

著录项

  • 作者

    Ihnatsenka, S.; Kirczenow, G.;

  • 作者单位
  • 年度 2011
  • 总页数
  • 原文格式 PDF
  • 正文语种 {"code":"en","name":"English","id":9}
  • 中图分类
  • 入库时间 2022-08-20 21:08:58

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