TABLE 1.
pigment (experiment) | retinal protonation | method | TD-B3LYP | SORCI+Q(6/6)b | MRCISD+Q(6/6)b |
---|---|---|---|---|---|
RH (500 nm) | PSBR | QM-none | 560 | 616 | 626 |
QM/MM | 503 | 495 | 499 | ||
SBR | QM-none | 408 | 328 | 319 | |
QM/MM | 429 | 336 | 324 | ||
HB (414 nm) | PSBR | QM-none | 634 | 556 | 546 |
QM/MM | 488 | 424 | 448 | ||
SBR | QM-none | 382 | 304 | 295 | |
QM/MM | 402 | 318 | 304 | ||
MUV (359 nm) | PSBR | QM-none | 596 | 550 | 541 |
QM/MM | 469 | 430 | 447 | ||
SBR | QM-none | 396 | 328 | 322 | |
QM/MM | 409 | 335 | 321 |
S1 and S2 vertical excitation energies of SBR are very close to each other. Only the absorbing state of SBR is given for relating the calculations with the experiments. The calculated oscillator strengths of the first absorbing state are 1.2–2.0 for both PSBR and SBR.
Estimated errors in SORCI+Q and MRCISD+Q vertical S1 excitation energies with the present computational settings (see ref 7) are 15 nm red shift for PSBR and 50 nm blue shift for SBR.