Thermal expansion in single-walled carbon nanotubes and graphene: Nonequilibrium Green’s function approach

TLDR

The study employs the nonequilibrium Green’s function method to calculate the coefficient of thermal expansion in single‑walled carbon nanotubes and graphene, examining size effects and the competition among vibrational modes. Atoms expand about 1 % from equilibrium even at 0 K due to zero‑point motion and nonlinear interactions; the axial CTE of SWCNTs remains positive over all temperatures while the radial CTE is negative at low temperatures, and graphene’s CTE is highly substrate‑dependent—without a substrate it is strongly negative at low temperatures and near zero at high temperatures (≈ −6 × 10⁻⁶ K⁻¹ at 300 K), whereas even a weak substrate suppresses the negative region and a strong substrate makes the CTE positive throughout, reaching ≈ 2.0 × 10⁻⁵ K⁻¹ at high temperatures. Published in Nanotechnology, vol.

Abstract

The nonequilibrium Green's function method is applied to investigate the coefficient of thermal expansion (CTE) in single-walled carbon nanotubes (SWCNT) and graphene. It is found that atoms expand about 1% from equilibrium positions even at $T=0\text{ }\text{K}$, resulting from the interplay between quantum zero-point motion and nonlinear interaction. The CTE in SWCNT of different sizes is studied and analyzed in terms of the competition between various vibration modes. As a result of this competition, the axial CTE is positive in the whole temperature range, while the radial CTE is negative at low temperatures. In graphene, the CTE is very sensitive to the substrate. Without substrate, CTE has large negative region at low temperatures and very small value at high-temperature limit, and the value of CTE at 300 K is $\ensuremath{-}6\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}6}\text{ }{\text{K}}^{\ensuremath{-}1}$ which is very close to a recent experimental result, $\ensuremath{-}7\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}6}\text{ }{\text{K}}^{\ensuremath{-}1}$ [Nat. Nanotechnol. 10, 1038 (2009)]. A very weak substrate interaction (about 0.06% of the in-plane interaction) can largely reduce the negative CTE region and greatly enhance the value of CTE. If the substrate interaction is strong enough, the CTE will be positive in whole temperature range and the saturate value at high temperatures reaches $2.0\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}5}\text{ }{\text{K}}^{\ensuremath{-}1}$.