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半导体石墨烯纳米带的电子结构与稳定性

Electronic structure and stability of semiconducting graphene nanoribbons.

作者信息

Barone Verónica, Hod Oded, Scuseria Gustavo E

机构信息

Department of Chemistry, Rice University, Houston, Texas 77005-1892, USA.

出版信息

Nano Lett. 2006 Dec;6(12):2748-54. doi: 10.1021/nl0617033.

Abstract

We present a systematic density functional theory study of the electronic properties, optical spectra, and relative thermodynamic stability of semiconducting graphene nanoribbons. We consider ribbons with different edge nature including bare and hydrogen-terminated ribbons, several crystallographic orientations, and widths up to 3 nm. Our results can be extrapolated to wider ribbons providing a qualitative way of determining the electronic properties of ribbons with widths of practical significance. We predict that in order to produce materials with band gaps similar to Ge or InN, the width of the ribbons must be between 2 and 3 nm. If larger bang gap ribbons are needed (like Si, InP, or GaAs), their width must be reduced to 1-2 nm. According to the extrapolated inverse power law obtained in this work, armchair carbon nanoribbons of widths larger than 8 nm will present a maximum band gap of 0.3 eV, while for ribbons with a width of 80 nm the maximum possible band gap is 0.05 eV. For chiral nanoribbons the band gap oscillations rapidly vanish as a function of the chiral angle indicating that a careful design of their crystallographic nature is an essential ingredient for controlling their electronic properties. Optical excitations show important differences between ribbons with and without hydrogen termination and are found to be sensitive to the carbon nanoribbon width. This should provide a practical way of revealing information on their size and the nature of their edges.

摘要

我们对半导体石墨烯纳米带的电子性质、光谱和相对热力学稳定性进行了系统的密度泛函理论研究。我们考虑了具有不同边缘性质的纳米带,包括裸露的和氢终止的纳米带、几种晶体取向以及宽度达3纳米的纳米带。我们的结果可以外推到更宽的纳米带,从而提供一种定性确定具有实际意义宽度的纳米带电子性质的方法。我们预测,为了制备具有与锗或氮化铟类似带隙的材料,纳米带的宽度必须在2至3纳米之间。如果需要更大带隙的纳米带(如硅、磷化铟或砷化镓),其宽度必须减小到1至2纳米。根据这项工作中得到的外推反幂律,宽度大于8纳米的扶手椅型碳纳米带将呈现最大0.3电子伏特的带隙,而对于宽度为80纳米的纳米带,最大可能带隙为0.05电子伏特。对于手性纳米带,带隙振荡随手性角的变化迅速消失,这表明仔细设计其晶体性质是控制其电子性质的关键因素。光学激发显示了有氢终止和无氢终止的纳米带之间的重要差异,并且发现对碳纳米带宽度敏感。这应该提供一种揭示其尺寸和边缘性质信息的实用方法。

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