Graphdiyne nanoribbons with open hexagonal rings: Existence of topological unprotected edge states

被引:16
作者
Chen, Cong [1 ]
Li, Jin [2 ,3 ]
Sheng, Xian-Lei [1 ]
机构
[1] Beihang Univ, Dept Phys, Minist Educ, Key Lab Micronano Measurement Manipulat & Phys, Beijing 100191, Peoples R China
[2] Xiangtan Univ, Lab Quantum Engn & Micronano Energy Technol, Xiangtan 411105, Hunan, Peoples R China
[3] Xiangtan Univ, Sch Phys & Optoelect, Xiangtan 411105, Hunan, Peoples R China
关键词
Graphdiyne nanoribbon; Tunable band gap; Topological unprotected edge states; First-principles calculations; ELECTRONIC-STRUCTURES; CARBON; GRAPHYNE; SCHEMES; SHEET;
D O I
10.1016/j.physleta.2017.08.034
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
Using first principles calculations, we studied a new class of graphdiyne nanoribbons (GDYNR) with open hexagonal rings on the edges. To avoid the effects from dangling bond, hydrogen or oxygen atoms were absorbed on the edges. There are two kinds of GDYNR depending on the edge structures, armchair and zigzag. The electronic structures show that all of them are semiconductors. The band gap can be tuned by the width of GDYNR. As the width of nanoribbons increases, the energy gap decreases firstly and then increases, and reaches a minimum gap for both kinds. To understand the intriguing phenomenon, we constructed a tight-binding model for GDYNR and found that the existence of the minimum of the energy gap is due to the competition between the interaction within the two edges and the coupling in between. Furthermore, topological unprotected edge states are found in the band structure of a semi infinite system by calculating surface Green's function. If GDYNR could be synthesized in experiments, it would be useful for the nanodevices in the future. (C) 2017 Elsevier B.V. All rights reserved.
引用
收藏
页码:3337 / 3341
页数:5
相关论文
共 45 条
[1]   Structures, stabilities and electronic properties of graphdiyne nanoribbons [J].
Bai, Hongcun ;
Zhu, Ying ;
Qiao, Weiye ;
Huang, Yuanhe .
RSC ADVANCES, 2011, 1 (05) :768-775
[2]   IMPROVED TETRAHEDRON METHOD FOR BRILLOUIN-ZONE INTEGRATIONS [J].
BLOCHL, PE ;
JEPSEN, O ;
ANDERSEN, OK .
PHYSICAL REVIEW B, 1994, 49 (23) :16223-16233
[3]   The electronic properties of graphene [J].
Castro Neto, A. H. ;
Guinea, F. ;
Peres, N. M. R. ;
Novoselov, K. S. ;
Geim, A. K. .
REVIEWS OF MODERN PHYSICS, 2009, 81 (01) :109-162
[4]  
CHEN X, 2015, SCI REP UK, V5
[5]   The geometric and electronic transitions in body-centered-tetragonal C8: A first principle study [J].
Cui, Hui-Juan ;
Yan, Qing-Bo ;
Sheng, Xian-Lei ;
Wang, Dong-Lin ;
Zheng, Qing-Rong ;
Su, Gang .
CARBON, 2017, 120 :89-94
[6]   Strain-induced Dirac cone-like electronic structures and semiconductor-semimetal transition in graphdiyne [J].
Cui, Hui-Juan ;
Sheng, Xian-Lei ;
Yan, Qing-Bo ;
Zheng, Qing-Rong ;
Su, Gang .
PHYSICAL CHEMISTRY CHEMICAL PHYSICS, 2013, 15 (21) :8179-8185
[7]  
Cui N.J., 2015, COMP MATER SCI, V98, P129
[8]  
Datta S., 1997, Electronic Transport in Mesoscopic Systems, DOI DOI 10.1063/1.2807624
[9]   Diamond: Electronic Ground State of Carbon at Temperatures Approaching 0 K [J].
Grochala, Wojciech .
ANGEWANDTE CHEMIE-INTERNATIONAL EDITION, 2014, 53 (14) :3680-3683
[10]   Homo Citans and Carbon Allotropes: For an Ethics of Citation [J].
Hoffmann, Roald ;
Kabanov, Artyom A. ;
Golov, Andrey A. ;
Proserpio, Davide M. .
ANGEWANDTE CHEMIE-INTERNATIONAL EDITION, 2016, 55 (37) :10962-10976