Table 1. The number of hops n, the number of used hopping sites ν, and the mean time required for each individual charge hopping τ = t/n.
| Carrier | F1/2 (V1/2cm−1/2) | n | ν | τ (ps) |
|---|---|---|---|---|
| Hole (with energetic disorder) | 300 | 220,324 | 1,265 | 2.6 |
| Hole (with energetic disorder) | 1300 | 1,022 | 266 | 4.3 |
| Electron (with energetic disorder) | 300 | 128,683 | 1,176 | 58.8 |
| Electron (with energetic disorder) | 1300 | 1,136 | 185 | 74.9 |
| Hole (without energetic disorder) | 300 | 4,729 | 1,257 | 0.4 |
| Hole (without energetic disorder) | 1300 | 405 | 235 | 0.9 |
| Electron (without energetic disorder) | 300 | 12,584 | 1,325 | 5.2 |
| Electron (without energetic disorder) | 1300 | 507 | 179 | 19.4 |
Intermolecular packing effect on λ is considered in all cases.
All of the values are the averages of 10,000 trials of the kinetic Monte Carlo simulation.