石墨烯中C - cite空位缺陷的第一性原理研究

H. K. Neupane, N. Adhikari
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引用次数: 0

摘要

利用计算工具Quantum ESPRESSO (QE)代码,在密度泛函理论(DFT)的框架下,通过第一性原理计算研究了水吸附石墨烯(wad - G)、水吸附石墨烯(1Catom-vacancy - wad - G)中的单碳(1C)原子空位缺陷和水吸附石墨烯(2Catom-vacancy - wad - G)材料中的双碳(2C)原子空位缺陷的电子和磁性。我们计算了wad - G、1catom -空位- wad - G和2catom -空位- wad - G材料的结合能,发现非缺陷几何比空位缺陷几何更紧凑。从能带结构计算中,我们发现wad - G是零带隙半导体,而1catom -空位- wad - G和2catom -空位- wad - G材料具有金属性质。因此,零带隙半导体由于其结构中的C位空位缺陷而转变为金属性质。利用态密度(DOS)和偏态密度(PDOS)计算方法研究了wad - G及其C位空位缺陷材料的磁性能。我们发现wad - G是一种非磁性材料。wad - G石墨烯表面的1C原子空位缺陷是通过两个悬空键的重键诱导磁化,并通过剩余的不饱和悬空键获得显著的磁矩(0.11µB/ cell)。但是,石墨烯表面2C原子空位缺陷的磁矩值(+0.03µB/ cell)比1C原子空位缺陷低,这是由于结构中没有悬空键的存在。因此,非磁性的wad - G由于在wad - G结构中存在C位空位缺陷而转变为磁性的1atom -空位- wad - G和2atom -空位- wad - G材料。缺陷结构中,碳原子的2p轨道对磁矩的贡献最大。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
First-principles study of C cites vacancy defects in water adsorbed Graphene
 The electronic and magnetic properties of water adsorbed graphene (wad – G), single carbon (1C) atom vacancy defects in water adsorbed graphene (1Catom-vacancy – wad – G) and double carbon (2C) atoms vacancy defects in water adsorbed graphene (2Catom-vacancy – wad – G) materials are studied by first-principles calculations within the frame work of density functional theory (DFT) using computational tool Quantum ESPRESSO (QE) code. We have calculated the binding energy of wad – G, 1Catom-vacancy – wad – G and 2Catom-vacancy – wad – G materials, and then found that non-defects geometry is more compact than vacancy defects geometries. From band structure calculations, we found that wad – G is zero band gap semiconductor, but 1Catom-vacancy – wad – G and, 2Catom-vacancy – wad – G materials have metallic properties. Hence, zero band gap semiconductor changes to metallic nature due to C sites vacancy defects in its structures. We have investigated the magnetic properties of wad – G and its C sites vacancy defects materials by using Density of States (DOS) and Partial Density of States (PDOS) calculations. We found that wad – G is non- magnetic material. 1C atom vacancy defects in graphene surface of wad – G is induced magnetization by the re-bonding of two dangling bonds and acquiring significant magnetic moment (0.11 µB/ cell) through remaining unsaturated dangling bond. But, 2C atoms vacancy defects in graphene surface of wad – G induced low value of magnetic moment (+0.03 µB/ cell) than 1C atom vacancy defects in structure, which is due to no dangling bonds present in the structure. Therefore, non-magnetic, wad – G changes to magnetic, 1Catom-vacancy – wad – G and, 2Catom-vacancy – wad – G materials due to C sites vacancy defects in wad – G structure. The 2p orbital of carbon atoms has main contribution of magnetic moment in defects structures.
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