Mobility in semiconducting carbon nanotubes at finite carrier density
arXiv:cond-mat/0510638 · doi:10.1021/nl052044h
Abstract
Carbon nanotube field-effect transistors operate over a wide range of electron or hole density, controlled by the gate voltage. Here we calculate the mobility in semiconducting nanotubes as a function of carrier density and electric field, for different tube diameters and temperature. The low-field mobility is a non-monotonic function of carrier density, and varies by as much as a factor of 4 at room temperature. At low density, with increasing field the drift velocity reaches a maximum and then exhibits negative differential mobility, due to the non-parabolicity of the bandstructure. At a critical density 0.35-0.5 electrons/nm, the drift velocity saturates at around one third of the Fermi velocity. Above , the velocity increases with field strength with no apparent saturation.
5 pages, 4 figures
References in corpus (7)
- Electron-Phonon Scattering in Metallic Single-Walled Carbon Nanotubes
- High-Field, Quasi-Ballistic Transport in Short Carbon Nanotubes
- Band Structure, Phonon Scattering and the Ultimate Performance of Single-Walled Carbon Nanotube Transistors
- Electron-phonon effects and transport in carbon nanotubes
- Electric Field-Dependent Charge-Carrier Velocity in Semiconducting Carbon Nanotubes
- Transport in Nanotubes: Effect of Remote Impurity Scattering
- Jahn-Teller instability in C6H6+ and C6H6- revisited
Cited by in corpus (8)
- Non-equilibrium Green's function treatment of phonon scattering in carbon nanotube transistors
- Multi-Band Mobility in Semiconducting Carbon Nanotubes
- Strong mobility degradation in ideal graphene nanoribbons due to phonon scattering
- Deformation Potential Carrier-Phonon Scattering in Semiconducting Carbon Nanotube Transistors
- Atomistic investigation of low-field mobility in graphene nanoribbons
- Microwave Rectification by a Carbon Nanotube Schottky Diode
- Shot noise suppression in quasi one-dimensional Field Effect Transistors
- Exciton dissociation in two-dimensional transition metal dichalcogenides: Excited states and substrate effects