Table 3. Hf2CO2 carrier mobility.
| Carrier type | ![]() |
![]() |
E1x | E1y | Cx | Cy | μx | μy |
|---|---|---|---|---|---|---|---|---|
| (eV) | (Jm−2) | (103 cm2V−1s−1) | ||||||
| e | 0.231 | 2.162 | 10.57 | 7.101 | 293.6 | 291.0 | 0.329 | 0.077 |
| h (upper) | 0.423 | 0.164 | 7.636 | 2.297 | 293.6 | 291.0 | 0.924 | 26.0 |
| h (lower) | 0.164 | 0.414 | 2.023 | 7.422 | 293.6 | 291.0 | 34.3 | 1.00 |
Carrier types “e” and “h” denote “electron” and “hole,” respectively.
and
are the effective masses along the zigzag (x-) and armchair (y-) directions, respectively. E1x and E1y are the deformation potential constants, and Cx and Cy are the elastic moduli. μx and μy are the room-temperature carrier mobilities.

