Abstract
In the previous chapters, we have largely focused on the role of transmission between CNTs and its effect on the conductance of the network as a whole.
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Notes
- 1.
Taking the MLWF centres from an isolated molecule is an excellent approximation: when adsorbed on the CNT, the MLWF centres of the water molecule are found to change by less than \(3\times 10^{-3}\,{\AA }\).
- 2.
This method cannot determine charge transfer that remains localised, however localised charge transfer does not contribute additional conductance.
- 3.
See Appendix D for a definition of the local density of states.
- 4.
The water geometry was generated using classical molecular dynamics as implemented in the Gromacs 4.5.5 package [35–38] with the GROMOS96 force field and 43a1 parameter set [39] and SPC water model [40] using NVT dynamics [41] at \(300 {\mathrm{{K}}}\) for \(20 {\mathrm{{ps}}}\). The water cluster was chosen as the first hydration shell surrounding a fully hydrated (10, 0) CNT. The electronic structure was calculated using onetep.
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Bell, R.A. (2015). Charge Doping in Water-Adsorbed Carbon Nanotubes. In: Conduction in Carbon Nanotube Networks. Springer Theses. Springer, Cham. https://doi.org/10.1007/978-3-319-19965-8_8
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