空位诱导的单层石墨烯电子-声子相互作用

Kamal Hosen, Biazid Kabir Moghal, A. Islam, M. S. Islam
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引用次数: 2

摘要

在石墨烯蜂窝结构中,声子粒子与电子强烈耦合,因此石墨烯结构的任何变化都会改变电子-声子(e-ph)相互作用,从而对石墨烯的电子和振动特性产生令人印象深刻的影响。在本文中,我们利用基于密度泛函理论的第一性原理计算报告了空位缺陷单层石墨烯的电子-声子相互作用。本文发现,空位缺陷在石墨烯结构中引入了带隙。在空位缺陷的石墨烯中,ZA声子模式在低频区向下移动,el-ph耦合系数从0.0035增加到0.30,高斯展宽0.5 Ry,表明空位缺陷增强了石墨烯结构中高频声子的弹道输运。同样,从拉曼光谱中发现,由于空位缺陷的存在,g峰从1607 cm - 1的频率转移到1704 cm - 1,并且在无序石墨烯中振动模式具有红外活性,而在原始石墨烯中则没有红外活性。因此,本文对空位诱导石墨烯结构的电子和振动特性有了深入的了解。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Vacancy Induced Electron-Phonon Interaction of Single Layer Graphene
In graphene honeycomb structure, the phonon particles are strongly coupled with the electrons, therefore any change in the structure of graphene changes the electron-phonon (e-ph) interaction and consequently it has an impressive effect on the electronic and vibrational properties of graphene. Here in this paper, we report the electron-phonon interaction of vacancy defected single layer graphene using first principle calculations based on density functional theory. In this paper, it has been found that vacancy defect introduces a band gap in the graphene structure. In vacancy defected graphene, the ZA phonon modes are shifted downward in the lower frequency region and the el-ph coupling coefficient increases from 0.0035 to 0.30 at Gaussian Broadening of 0.5 Ry which indicates that vacancy defect enhances a ballistic transports of the high-frequency phonons in graphene structure. Again, from Raman spectrum it has found that the G-peak shifts from the frequency of 1607 cm−1to 1704 cm 1due to the presence of vacancy defect and the vibrational modes are IR active in disordered graphene where they are not IR active in case of pristine graphene. Thus this paper gives a deep insight about the electronic and vibrational properties of vacancy induced graphene structure.
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