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首页> 外文期刊>Physical Review. B, Condensed Matter >First-principles calculations of the geometry and electronic structure of electron- and hole-doped C_(60) in the field-effect transistor structure
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First-principles calculations of the geometry and electronic structure of electron- and hole-doped C_(60) in the field-effect transistor structure

机译:场效应晶体管结构中电子和空穴掺杂C_(60)的几何和电子结构的第一性原理计算

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We investigate the geometry and electronic structure of field-effect-doped C_(60) by carrying out first-principles calculations based on the density-functional theory. To reproduce field-effect doping, we employ a structural model which consists of a single C_(60) (111) layer and an electrode layer. In this model, we assume that the carrier concentration is higher than one electron or hole per unit cell. We find that the charge distribution on the electrode side hemisphere of the C_(60) molecule, say the north hemisphere, is changed by field-effect doping while that on the south hemisphere is hardly changed. In particular, on the hexagonal face nearest to the electrode, the π-like electron density is considerably increased and decreased in electron- and hole-doped C_(60), respectively. Therefore, the C-C bonds on this face are elongated with increasing the carrier concentration both in electron- and hole-doped C_(60). Furthermore, it is found that the potential energy induced by field-effect doping is large enough to change the band dispersion and the density of states. In addition, we discuss the charge distribution at lower carrier concentrations with two models; one is the model consisting of three C_(60) layers and the other is the continuum model.
机译:我们通过基于密度泛函理论的第一性原理计算,研究了场效应掺杂的C_(60)的几何结构和电子结构。为了重现场效应掺杂,我们采用了由单个C_(60)(111)层和一个电极层组成的结构模型。在此模型中,我们假设载流子浓度高于每个晶胞一个电子或一个空穴。我们发现,C_(60)分子的电极侧半球(即北半球)的电荷分布通过场效应掺杂而改变,而南半球的电荷分布几乎不变。特别地,在最靠近电极的六边形表面上,π型电子密度在电子和空穴掺杂的C_(60)中分别显着增加和降低。因此,该面的C-C键随着电子和空穴掺杂C_(60)中载流子浓度的增加而延长。此外,发现由场效应掺杂引起的势能足够大,以改变带分散和状态密度。另外,我们用两种模型讨论了在较低载流子浓度下的电荷分布。一种是由三个C_(60)层组成的模型,另一种是连续体模型。

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