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The ground state of graphene and graphene disordered by vacancies

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The ground state of graphene and graphene disordered by vacancies. / Kheirabadi, Narjes; Shafiekhani, A.
In: Physica E: Low-dimensional Systems and Nanostructures, Vol. 47, 01.2013, p. 309-315.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

Kheirabadi, N & Shafiekhani, A 2013, 'The ground state of graphene and graphene disordered by vacancies', Physica E: Low-dimensional Systems and Nanostructures, vol. 47, pp. 309-315. https://doi.org/10.1016/j.physe.2012.09.022

APA

Kheirabadi, N., & Shafiekhani, A. (2013). The ground state of graphene and graphene disordered by vacancies. Physica E: Low-dimensional Systems and Nanostructures, 47, 309-315. https://doi.org/10.1016/j.physe.2012.09.022

Vancouver

Kheirabadi N, Shafiekhani A. The ground state of graphene and graphene disordered by vacancies. Physica E: Low-dimensional Systems and Nanostructures. 2013 Jan;47:309-315. Epub 2010 Apr 17. doi: 10.1016/j.physe.2012.09.022

Author

Kheirabadi, Narjes ; Shafiekhani, A. / The ground state of graphene and graphene disordered by vacancies. In: Physica E: Low-dimensional Systems and Nanostructures. 2013 ; Vol. 47. pp. 309-315.

Bibtex

@article{9a50fa520a624caf942c4263e59521e3,
title = "The ground state of graphene and graphene disordered by vacancies",
abstract = "Graphene clusters consisting of 24 to 150 carbon atoms and hydrogen termination at the zigzag boundary edges have been studied, as well as clusters disordered by vacancy(s). Density Function Theory and Gaussian03 software were used to calculate graphene relative stability, desorption energy, band gap, density of states, surface shape, dipole momentum and electrical polarization of all clusters by applying the hybrid exchange-correlation functional Beke-Lee-Yang-Parr. Furthermore, infrared frequencies were calculated for two of them. Different basis sets, 6-31g**, 6-31g* and 6-31g, depending on the sizes of clusters are considered to compromise the effect of this selection on the calculated results. We found that relative stability and the gap decreases according to the size increase of the graphene cluster. Mulliken charge variation increase with the size. For about 500 carbon atoms, a zero HOMO-LUMO gap amount is predicted. Vacancy generally reduces the stability and having vacancy affects the stability differently according to the location of vacancies. Surface geometry of each cluster depends on the number of vacancies and their locations. The energy gap changes as with the location of vacancies in each cluster. The dipole momentum is dependent on the location of vacancies with respect to one another. The carbon-carbon length changes according to each covalence band distance from the boundary and vacancies. Two basis sets, 6-31g* and 6-31g**, predict equal amount for energy, gap and surface structure, but charge distribution results are completely different.",
keywords = "cond-mat.mes-hall",
author = "Narjes Kheirabadi and A. Shafiekhani",
year = "2013",
month = jan,
doi = "10.1016/j.physe.2012.09.022",
language = "English",
volume = "47",
pages = "309--315",
journal = "Physica E: Low-dimensional Systems and Nanostructures",
issn = "1386-9477",
publisher = "Elsevier",

}

RIS

TY - JOUR

T1 - The ground state of graphene and graphene disordered by vacancies

AU - Kheirabadi, Narjes

AU - Shafiekhani, A.

PY - 2013/1

Y1 - 2013/1

N2 - Graphene clusters consisting of 24 to 150 carbon atoms and hydrogen termination at the zigzag boundary edges have been studied, as well as clusters disordered by vacancy(s). Density Function Theory and Gaussian03 software were used to calculate graphene relative stability, desorption energy, band gap, density of states, surface shape, dipole momentum and electrical polarization of all clusters by applying the hybrid exchange-correlation functional Beke-Lee-Yang-Parr. Furthermore, infrared frequencies were calculated for two of them. Different basis sets, 6-31g**, 6-31g* and 6-31g, depending on the sizes of clusters are considered to compromise the effect of this selection on the calculated results. We found that relative stability and the gap decreases according to the size increase of the graphene cluster. Mulliken charge variation increase with the size. For about 500 carbon atoms, a zero HOMO-LUMO gap amount is predicted. Vacancy generally reduces the stability and having vacancy affects the stability differently according to the location of vacancies. Surface geometry of each cluster depends on the number of vacancies and their locations. The energy gap changes as with the location of vacancies in each cluster. The dipole momentum is dependent on the location of vacancies with respect to one another. The carbon-carbon length changes according to each covalence band distance from the boundary and vacancies. Two basis sets, 6-31g* and 6-31g**, predict equal amount for energy, gap and surface structure, but charge distribution results are completely different.

AB - Graphene clusters consisting of 24 to 150 carbon atoms and hydrogen termination at the zigzag boundary edges have been studied, as well as clusters disordered by vacancy(s). Density Function Theory and Gaussian03 software were used to calculate graphene relative stability, desorption energy, band gap, density of states, surface shape, dipole momentum and electrical polarization of all clusters by applying the hybrid exchange-correlation functional Beke-Lee-Yang-Parr. Furthermore, infrared frequencies were calculated for two of them. Different basis sets, 6-31g**, 6-31g* and 6-31g, depending on the sizes of clusters are considered to compromise the effect of this selection on the calculated results. We found that relative stability and the gap decreases according to the size increase of the graphene cluster. Mulliken charge variation increase with the size. For about 500 carbon atoms, a zero HOMO-LUMO gap amount is predicted. Vacancy generally reduces the stability and having vacancy affects the stability differently according to the location of vacancies. Surface geometry of each cluster depends on the number of vacancies and their locations. The energy gap changes as with the location of vacancies in each cluster. The dipole momentum is dependent on the location of vacancies with respect to one another. The carbon-carbon length changes according to each covalence band distance from the boundary and vacancies. Two basis sets, 6-31g* and 6-31g**, predict equal amount for energy, gap and surface structure, but charge distribution results are completely different.

KW - cond-mat.mes-hall

U2 - 10.1016/j.physe.2012.09.022

DO - 10.1016/j.physe.2012.09.022

M3 - Journal article

VL - 47

SP - 309

EP - 315

JO - Physica E: Low-dimensional Systems and Nanostructures

JF - Physica E: Low-dimensional Systems and Nanostructures

SN - 1386-9477

ER -