Table 7.
State | Symm. | B3LYP[a] |
B2PLYP[b] |
HYBRID[b] |
Expt. |
|||
---|---|---|---|---|---|---|---|---|
ω | ν | ω | ν | ω | ν | ν | ||
Σg | 3466 | 3343 | 3477 | 3352 | 3463 | 3338 | 3332 | |
2278 | 2238 | 2234 | 2189 | 2243 | 2197 | 2189 | ||
915 | 901 | 908 | 890 | 894 | 872 | 872 | ||
Σu | 3467 | 3344 | 3478 | 3353 | 3465 | 3339 | 3334 | |
2111 | 2078 | 2064 | 2028 | 2064 | 2027 | 2022 | ||
∏g | 659 | 647 | 645 | 638 | 636 | 627 | 626 | |
529 | 522 | 507 | 512 | 485 | 491 | 483 | ||
∏u | 665 | 654 | 651 | 640 | 640 | 628 | 628 | |
237 | 237 | 231 | 232 | 221 | 222 | 220 |
The vibrational states are indicated as. DFT calculations were done in conjunction of the AVTZ basis set. Within the hybrid scheme, the harmonic wavenumbers, obtained at the AE-CCSD(T)/cc-pCVQZ level, were taken from Ref.61, and the anharmonic force-field calculated in this work at the B2PLYP/AVTZ level. The experimental values were taken from Refs.61 and63.
VPT2 values, no Fermi resonances identified with Martin's test.
GVPT2 values, one weakly interaction between and states.