scholarly journals Width-Dependent Band Gap in Armchair Graphene Nanoribbons Reveals Fermi Level Pinning on Au(111)

ACS Nano ◽  
2017 ◽  
Vol 11 (11) ◽  
pp. 11661-11668 ◽  
Author(s):  
Néstor Merino-Díez ◽  
Aran Garcia-Lekue ◽  
Eduard Carbonell-Sanromà ◽  
Jingcheng Li ◽  
Martina Corso ◽  
...  
2019 ◽  
Vol 7 (21) ◽  
pp. 6241-6245 ◽  
Author(s):  
Wei-Wei Yan ◽  
Xiao-Fei Li ◽  
Xiang-Hua Zhang ◽  
Xinrui Cao ◽  
Mingsen Deng

Boron adsorption induces a heavily localized state right at the Fermi level only in the family of W = 3p + 1 and thus spin-splitting occurs spontaneously.


2017 ◽  
Vol 139 (10) ◽  
pp. 3635-3638 ◽  
Author(s):  
Zongping Chen ◽  
Hai I. Wang ◽  
Joan Teyssandier ◽  
Kunal S. Mali ◽  
Tim Dumslaff ◽  
...  

2018 ◽  
Vol 9 (1) ◽  
Author(s):  
Gang Li ◽  
Ki-Young Yoon ◽  
Xinjue Zhong ◽  
Jianchun Wang ◽  
Rui Zhang ◽  
...  

2018 ◽  
Vol 787 ◽  
pp. 99-103
Author(s):  
Xian Bin Zhang ◽  
Ning Kang Deng ◽  
Wen Jie Wu ◽  
Xu Yan Wei ◽  
Guan Qi Wang

In this paper, the electronic structure in armchair graphene nanoribbons (AGNRs) and graphene nanoribbons doped B at the edge (B-AGNRs) are obtained based on the first principle theory. It shows that the band gap has the oscillation characteristic whose period is 3. The band gap oscillating characteristic gradually vanishes and tends to be stable after doping B at graphene nanoribbons edge. This provides a theoretical guidance for developing the stable graphene nanodevices.


2016 ◽  
Vol 46 (1) ◽  
pp. 340-346 ◽  
Author(s):  
Milad Zoghi ◽  
Arash Yazdanpanah Goharrizi ◽  
Mehdi Saremi

2016 ◽  
Vol 94 (2) ◽  
pp. 218-225 ◽  
Author(s):  
M. Khatun ◽  
Z. Kan ◽  
A. Cancio ◽  
C. Nelson

We explore a model of armchair graphene nanoribbons tuned by functionalizing the edge states. Edge modifications are modeled by changing the electronic energy of the edge states in specific periodic patterns. The model can be considered to mimic a controlled doping process with different elements. The band structure, density of states, conductance, and local density of states are calculated, using the tight binding approach, Green’s function methodology, and the Landauer formula. The results show interesting behaviors, which are considerably different from the properties of the perfect nanoribbons. The hybridization of conducting bands with non-conducting bands, which appear perfectly flat in the perfect ribbon, opens up and modifies gaps in conductance near the Fermi level. One particular pattern of edge functionalization causes a strong, symmetric, and systematic band gap change about the Fermi level, modifying the electronic characteristics in the energy dispersion, density of states, local density of states, and conductance.


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