Dirac cone manipulation via bismuth and oxygen intercalation underneath graphene on Re(0001)

A. A. Gogina, I. Klimovskikh, D. Estyunin, S. Filnov, A. Shikin
{"title":"Dirac cone manipulation via bismuth and oxygen intercalation underneath graphene on Re(0001)","authors":"A. A. Gogina, I. Klimovskikh, D. Estyunin, S. Filnov, A. Shikin","doi":"10.1063/5.0056673","DOIUrl":null,"url":null,"abstract":"This paper reports on an investigation by angle-resolved photoelectron spectroscopy of the graphene on Re(0001) sub- strate, after intercalation by bismuth atoms. Our results demonstrate that intercalation of Bi atoms restores the quasi-free-standing properties of graphene. Thus, the band structure of this system is characterized by a linear π-state dispersion near the K point of the Brillouin zone. The Dirac point shifts toward higher binding energies by approximately 0.4 eV, which is caused by charge transfer from Bi atoms to graphene. Besides we observed a band gap with a width of at least 0.4 eV. The possible reasons of the band gap in the system Gr/Bi/Re(0001) can be caused by hybridization of π-states of graphene with 5d-rhenium states and/or bismuth states or symmetry breaking of the sublattices of graphene. Moreover, the Dirac point position is found to be different depending on the intercalated atoms. Intercalation of the oxygen atoms underneath graphene after exposure to the air results in the appearance of the second π-state branch in the electronic structure. There are two Dirac cones in the ARPES image and for the first one the charge transfer from the Bi atoms leads to the Dirac point position below the Fermi level, i.e. to the n-doping of graphene. For the second one the Dirac point is located above the Fermi level resulting in p-doping that is caused by charge transfer between oxygen and graphene atoms.","PeriodicalId":405600,"journal":{"name":"PROCEEDINGS OF INTERNATIONAL CONGRESS ON GRAPHENE, 2D MATERIALS AND APPLICATIONS (2D MATERIALS 2019)","volume":"10 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2021-06-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"PROCEEDINGS OF INTERNATIONAL CONGRESS ON GRAPHENE, 2D MATERIALS AND APPLICATIONS (2D MATERIALS 2019)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1063/5.0056673","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

Abstract

This paper reports on an investigation by angle-resolved photoelectron spectroscopy of the graphene on Re(0001) sub- strate, after intercalation by bismuth atoms. Our results demonstrate that intercalation of Bi atoms restores the quasi-free-standing properties of graphene. Thus, the band structure of this system is characterized by a linear π-state dispersion near the K point of the Brillouin zone. The Dirac point shifts toward higher binding energies by approximately 0.4 eV, which is caused by charge transfer from Bi atoms to graphene. Besides we observed a band gap with a width of at least 0.4 eV. The possible reasons of the band gap in the system Gr/Bi/Re(0001) can be caused by hybridization of π-states of graphene with 5d-rhenium states and/or bismuth states or symmetry breaking of the sublattices of graphene. Moreover, the Dirac point position is found to be different depending on the intercalated atoms. Intercalation of the oxygen atoms underneath graphene after exposure to the air results in the appearance of the second π-state branch in the electronic structure. There are two Dirac cones in the ARPES image and for the first one the charge transfer from the Bi atoms leads to the Dirac point position below the Fermi level, i.e. to the n-doping of graphene. For the second one the Dirac point is located above the Fermi level resulting in p-doping that is caused by charge transfer between oxygen and graphene atoms.
查看原文
分享 分享
微信好友 朋友圈 QQ好友 复制链接
本刊更多论文
Re上石墨烯下铋和氧嵌入的狄拉克锥操纵(0001)
本文报道了用角分辨光电子能谱法研究了铋原子插层后石墨烯在Re(0001)衬底上的性能。我们的研究结果表明,Bi原子的插入恢复了石墨烯的准独立性质。因此,该体系的能带结构在布里渊区K点附近具有线性π态色散。Dirac点向更高结合能偏移了约0.4 eV,这是由Bi原子向石墨烯的电荷转移引起的。此外,我们还观察到一个宽度至少为0.4 eV的带隙。Gr/Bi/Re(0001)体系中出现带隙的可能原因是石墨烯π态与5d-铼态和/或铋态的杂化或石墨烯亚晶格的对称性破缺。此外,发现狄拉克点的位置随插入原子的不同而不同。氧原子在暴露于空气后嵌入石墨烯下,导致电子结构中出现第二π态分支。在ARPES图像中有两个狄拉克锥,对于第一个,来自Bi原子的电荷转移导致狄拉克点位置低于费米能级,即石墨烯的n掺杂。对于第二种,狄拉克点位于费米能级之上,导致p掺杂,这是由氧和石墨烯原子之间的电荷转移引起的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 去求助
来源期刊
自引率
0.00%
发文量
0
期刊最新文献
The second optical harmonic generation efficiency estimation in two-dimensional semiconductor heterostructures Ultrafast dynamics of the magneto-optical Kerr effect in multilayer TbCo/FeCo structures under the influence of femtosecond optical excitation Optical properties of multilayer heterostructures based on transition metal dichalcogenides The generation of THz radiation in layered transition metal dichalcogenides Quasi-one-dimensional chains of magnetic tunnel junctions as a source of THz radiation
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
现在去查看 取消
×
提示
确定
0
微信
客服QQ
Book学术公众号 扫码关注我们
反馈
×
意见反馈
请填写您的意见或建议
请填写您的手机或邮箱
已复制链接
已复制链接
快去分享给好友吧!
我知道了
×
扫码分享
扫码分享
Book学术官方微信
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术
文献互助 智能选刊 最新文献 互助须知 联系我们:info@booksci.cn
Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。
Copyright © 2023 Book学术 All rights reserved.
ghs 京公网安备 11010802042870号 京ICP备2023020795号-1