Table 2. Principal Components for the HFC A of [Lu(OAr*)3]− and Isotropic HFC A of [TbPc2]− at Various Levels of theory38,39,117,149 and Comparison with Experimental Results (expt.)181,182a.
[Lu(OAr*)3]− |
[TbPc2]− | ||||
---|---|---|---|---|---|
method | Axx | Ayy | Azz | A | |
TPSS | SR | 3192 | 3192 | 3148 | 190 |
cTPSS | SO | 3190 | 3190 | 3153 | 375 |
ωB97X-D | SR | 3489 | 3489 | 3456 | 136 |
ωB97X-D | SO | 3464 | 3464 | 3448 | 488 |
TMHF | SR | 3225 | 3225 | 3171 | 293 |
cTMHF | SO | 3208 | 3208 | 3161 | 526 |
Expt. | 3500 | 3500 | 3400 | 519 |
HFC is given in MHz. SR and SO denote scalar and spin–orbit relativistic results (x2c-TZVPall-2c/x2c-SVPall-2c basis), respectively.