Volume 3, Issue 3
Tight-Binding Calculation of Growth Mechanism of Graphene on Ni(111) Surface

Chen Zhou, Jing Hu, Yuan Tian, Qian-Ying Zhao, Ling Miu & Jian-Jun Jiang

J. At. Mol. Sci., 3 (2012), pp. 270-278.

Published online: 2012-03

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  • Abstract

The nucleation of graphene on Ni surface, as well as on the step, is studied using a tight binding method of SCC-DFTB. The result demonstrates that the fcc configuration has the lowest total energy and thus is the most stable one compared to the other two structures when benzene ring is absorbed on the Ni(111) surface. The activity of marginal growth graphene's carbon atoms decreases from the boundary to the center, when they are absorbed on the substrate. Graphene layer can grow continuously on step surface formed by intersection of Ni(111) and Ni(1$\bar{1}$1) surface. Meanwhile, a mismatch will occur between the graphene layer and Ni surface and thus leads to flaws when the layer grows larger. Reducing the mismatch between the graphene and the step surface will benefit the growth of graphene of large area and high quality.

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COPYRIGHT: © Global Science Press

  • Email address

zhouchen0331@gmail.com (Chen Zhou)

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@Article{JAMS-3-270, author = {Zhou , ChenHu , JingTian , YuanZhao , Qian-YingMiu , Ling and Jiang , Jian-Jun}, title = {Tight-Binding Calculation of Growth Mechanism of Graphene on Ni(111) Surface}, journal = {Journal of Atomic and Molecular Sciences}, year = {2012}, volume = {3}, number = {3}, pages = {270--278}, abstract = {

The nucleation of graphene on Ni surface, as well as on the step, is studied using a tight binding method of SCC-DFTB. The result demonstrates that the fcc configuration has the lowest total energy and thus is the most stable one compared to the other two structures when benzene ring is absorbed on the Ni(111) surface. The activity of marginal growth graphene's carbon atoms decreases from the boundary to the center, when they are absorbed on the substrate. Graphene layer can grow continuously on step surface formed by intersection of Ni(111) and Ni(1$\bar{1}$1) surface. Meanwhile, a mismatch will occur between the graphene layer and Ni surface and thus leads to flaws when the layer grows larger. Reducing the mismatch between the graphene and the step surface will benefit the growth of graphene of large area and high quality.

}, issn = {2079-7346}, doi = {https://doi.org/10.4208/jams.101411.111611a}, url = {http://global-sci.org/intro/article_detail/jams/8200.html} }
TY - JOUR T1 - Tight-Binding Calculation of Growth Mechanism of Graphene on Ni(111) Surface AU - Zhou , Chen AU - Hu , Jing AU - Tian , Yuan AU - Zhao , Qian-Ying AU - Miu , Ling AU - Jiang , Jian-Jun JO - Journal of Atomic and Molecular Sciences VL - 3 SP - 270 EP - 278 PY - 2012 DA - 2012/03 SN - 3 DO - http://doi.org/10.4208/jams.101411.111611a UR - https://global-sci.org/intro/article_detail/jams/8200.html KW - graphene, metallic substrate, surface structure, growth on step, tight binding approximation. AB -

The nucleation of graphene on Ni surface, as well as on the step, is studied using a tight binding method of SCC-DFTB. The result demonstrates that the fcc configuration has the lowest total energy and thus is the most stable one compared to the other two structures when benzene ring is absorbed on the Ni(111) surface. The activity of marginal growth graphene's carbon atoms decreases from the boundary to the center, when they are absorbed on the substrate. Graphene layer can grow continuously on step surface formed by intersection of Ni(111) and Ni(1$\bar{1}$1) surface. Meanwhile, a mismatch will occur between the graphene layer and Ni surface and thus leads to flaws when the layer grows larger. Reducing the mismatch between the graphene and the step surface will benefit the growth of graphene of large area and high quality.

Zhou , ChenHu , JingTian , YuanZhao , Qian-YingMiu , Ling and Jiang , Jian-Jun. (2012). Tight-Binding Calculation of Growth Mechanism of Graphene on Ni(111) Surface. Journal of Atomic and Molecular Sciences. 3 (3). 270-278. doi:10.4208/jams.101411.111611a
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