Ballistic transport and electrostatics in metallic carbon nanotubes
arXiv:cond-mat/0504004 · doi:10.1109/TNANO.2005.851409
Abstract
We calculate the current and electrostatic potential drop in metallic carbon nanotube wires self-consistently, by solving the Green's function and electrostatics equations in the ballistic case. About one tenth of the applied voltage drops across the bulk of a nanowire, independent of the lengths considered here. The remaining nine tenths of the bias drops near the contacts, thereby creating a non linear potential drop. The scaling of the electric field at the center of the nanotube with length (L) is faster than 1/L (roughly ). At room temperature, the low bias conductance of large diameter nanotubes is larger than due to occupation of non crossing subbands. The physics of conductance evolution with bias due to the transmission Zener tunneling in non crossing subbands is discussed.
References in corpus (7)
- Density functional method for nonequilibrium electron transport
- High-Field Electrical Transport in Single-Wall Carbon Nanotubes
- Electron-Phonon Scattering in Metallic Single-Walled Carbon Nanotubes
- Scanned Probe Microscopy of Electronic Transport in Carbon Nanotubes
- Two Dimensional Quantum Mechanical Modeling of Nanotransistors
- Current carrying capacity of carbon nanotubes
- Which nanowire couples better electrically to a metal contact: armchair or zigzag nanotube?