Table 4. Emission Energies of the matched and mismatched duplexes.
Vertical Emission Energies (VEE) and oscillator strengths (f) at the QM(PCM/M052X/6–31G(d) Linear Response (LR) level of theory are compared to those computed at the State Specific (SS)-PCM. Charge Transfer character (CT in a.u), radiative lifetime (τR in ns) and computed fluorescence lifetimes (c<τ> in ns) of the different minima for the different duplexes.
| (−)PBS | (+)PBS | Description. | LRVEE (eV) | LRf | LRCT | SSVEE (eV) | SSf | SSτR | c<τ> |
|---|---|---|---|---|---|---|---|---|---|
| AthGA | TCT | Min-ππ* | 3.28 | 0.07 | 0.03 | 3.20 | 0.05 | 74 | 13.4 |
| Min-CT (thG→A) | 3.77 | 0.01 | 0.58 | 2.53 | 0.00 | ||||
| TthGT | ACA | Min-ππ*modell | 3.43 | 0.08 | 0.01 | 3.32 | 0.05 | 64 | 9.7 |
| Min-CTmodel2 (thG→T) | 3.34 | 0.00 | 0.86 | 1.68 | 0.00 | ||||
| CthGC | GCG | Min-ππ* | 3.42 | 0.08 | 0.01 | 3.33 | 0.06 | 52 | 8.3 |
| Min-CT (thG→C) | a3.88 | 0.03 | 0.72 | 2.10 | 0.01 | ||||
| GthGG | CCC | Min-ππ* | 3.47 | 0.08 | 0.03 | 3.33 | 0.05 | 64 | 9.6 |
| Min-CT (G→thG) | 3.15 | 0.02 | −0.22 | 2.80 | 0.01 | ||||
| GthGG | CTC | Min-ππ* | b | ||||||
| Min-CT (G→thG) | 4.24 | 0.07 | −0.22 | 2.91 | 0.01 | 7000 | |||
| AthGA | TAT | Min-ππ* | 3.67 | 0.11 | 0.03 | 3.39 | 0.08 | 29 | 14.0 |
| Min-CT | c | ||||||||
| TthGT | ATA | g1Min-ππ* | 3.46 | 0.07 | 0.04 | 3.32 | 0.05 | 68 | 23.7 |
| g1Min-ct (thG→T) | 3.36 | 0.06 | 0.06 | 3.24 | 0.04 | ||||
| TthGT | AAA | g3Min-ππ* | 3.50 | 0.08 | 0.01 | 3.29 | 0.06 | 62 | 22.8 |
| g1Min-ct (thG→T) | 2.93 | 0.01 | 0.16 | 2.80 | 0.01 | ||||
| TthGT | AGA | Min-ππ* | 3.63 | 0.11 | 0.00 | 3.33 | 0.08 | 28 | 2.8 |
| Min-CT | c |
Notes: a) No real minimum but a low energy gradient region was found, b) no clear ππ * minimum was found, c) no clear CT minimum was located. The radiative lifetime (τR) was estimated by using a simplified version of the Strickler-Berg formula: with , where ΔE is the vertical emission energy and the dipole moment of the transition. The computed lifetime is calculated by: c<τ> = kR×QY, where QY is the experimental quantum yield. Further details on the calculations are given in section 4 of SI.