Using the valence force field model of Perebeinos and Tersoff Phys. Rev. B
\bf79, 241409(R) (2009), different energy modes of suspended graphene
subjected to tensile or compressive strain are studied. By carrying out Monte
Carlo simulations it is found that: i) only for small strains (\$|\varepsilon|
0.02\$) the total energy is symmetrical in the strain, while it
behaves completely different beyond this threshold; ii) the important energy
contributions in stretching experiments are stretching, angle bending,
out-of-plane term and a term that provides repulsion against \$\pi-\pi\$
misalignment; iii) in compressing experiments the two latter terms increase
rapidly and beyond the buckling transition stretching and bending energies are
found to be constant; iv) from stretching-compressing simulations we calculated
the Young modulus at room temperature 350\$\pm3.15\$\,N/m, which is in good
agreement with experimental results (340\$\pm50\$\,N/m) and with ab-initio
results 322-353\,N/m; v) molar heat capacity is estimated to be
24.64\,J/mol\$^-1\$K\$^-1\$ which is comparable with the Dulong-Petit value,
i.e. 24.94\,J/mol\$^-1\$K\$^-1\$ and is almost independent of the strain; vi)
non-linear scaling properties are obtained from height-height correlations at
finite temperature; vii) the used valence force field model results in a
temperature independent bending modulus for graphene, and viii) the Gruneisen
parameter is estimated to be 0.64.
%0 Generic
%1 Lajevardipour2012Thermomechanical
%A Lajevardipour, A.
%A Neek-Amal, M.
%A Peeters, F. M.
%D 2012
%K graphene
%T Thermomechanical properties of graphene: valence force field model approach
%U http://arxiv.org/abs/1203.0610
%X Using the valence force field model of Perebeinos and Tersoff Phys. Rev. B
\bf79, 241409(R) (2009), different energy modes of suspended graphene
subjected to tensile or compressive strain are studied. By carrying out Monte
Carlo simulations it is found that: i) only for small strains (\$|\varepsilon|
0.02\$) the total energy is symmetrical in the strain, while it
behaves completely different beyond this threshold; ii) the important energy
contributions in stretching experiments are stretching, angle bending,
out-of-plane term and a term that provides repulsion against \$\pi-\pi\$
misalignment; iii) in compressing experiments the two latter terms increase
rapidly and beyond the buckling transition stretching and bending energies are
found to be constant; iv) from stretching-compressing simulations we calculated
the Young modulus at room temperature 350\$\pm3.15\$\,N/m, which is in good
agreement with experimental results (340\$\pm50\$\,N/m) and with ab-initio
results 322-353\,N/m; v) molar heat capacity is estimated to be
24.64\,J/mol\$^-1\$K\$^-1\$ which is comparable with the Dulong-Petit value,
i.e. 24.94\,J/mol\$^-1\$K\$^-1\$ and is almost independent of the strain; vi)
non-linear scaling properties are obtained from height-height correlations at
finite temperature; vii) the used valence force field model results in a
temperature independent bending modulus for graphene, and viii) the Gruneisen
parameter is estimated to be 0.64.
@misc{Lajevardipour2012Thermomechanical,
abstract = {Using the valence force field model of Perebeinos and Tersoff [Phys. Rev. B
{\bf79}, 241409(R) (2009)], different energy modes of suspended graphene
subjected to tensile or compressive strain are studied. By carrying out Monte
Carlo simulations it is found that: i) only for small strains (\$|\varepsilon|
\lessapprox 0.02\$) the total energy is symmetrical in the strain, while it
behaves completely different beyond this threshold; ii) the important energy
contributions in stretching experiments are stretching, angle bending,
out-of-plane term and a term that provides repulsion against \$\pi-\pi\$
misalignment; iii) in compressing experiments the two latter terms increase
rapidly and beyond the buckling transition stretching and bending energies are
found to be constant; iv) from stretching-compressing simulations we calculated
the Young modulus at room temperature 350\$\pm3.15\$\,N/m, which is in good
agreement with experimental results (340\$\pm50\$\,N/m) and with ab-initio
results [322-353]\,N/m; v) molar heat capacity is estimated to be
24.64\,J/mol\$^{-1}\$K\$^{-1}\$ which is comparable with the Dulong-Petit value,
i.e. 24.94\,J/mol\$^{-1}\$K\$^{-1}\$ and is almost independent of the strain; vi)
non-linear scaling properties are obtained from height-height correlations at
finite temperature; vii) the used valence force field model results in a
temperature independent bending modulus for graphene, and viii) the Gruneisen
parameter is estimated to be 0.64.},
added-at = {2019-02-23T22:09:48.000+0100},
archiveprefix = {arXiv},
author = {Lajevardipour, A. and Neek-Amal, M. and Peeters, F. M.},
biburl = {https://www.bibsonomy.org/bibtex/2e3071cd57df0458fd9327f144ef39327/cmcneile},
citeulike-article-id = {12628588},
citeulike-linkout-0 = {http://arxiv.org/abs/1203.0610},
citeulike-linkout-1 = {http://arxiv.org/pdf/1203.0610},
day = 3,
eprint = {1203.0610},
interhash = {a7b5004261e96921964dec344025d7bb},
intrahash = {e3071cd57df0458fd9327f144ef39327},
keywords = {graphene},
month = mar,
posted-at = {2013-09-16 17:41:50},
priority = {2},
timestamp = {2019-02-23T22:15:27.000+0100},
title = {{Thermomechanical properties of graphene: valence force field model approach}},
url = {http://arxiv.org/abs/1203.0610},
year = 2012
}