Photophysical properties of the ITI photoswitches substituted in the X positiona.
| ||||||||
|---|---|---|---|---|---|---|---|---|
| X | λ max,Z (nm) | λ max,E (nm) | Φ Z–E (%) | ε Z (M−1 cm−1) | ΔG°# (kcal mol−1) calc. | ΔG°# (kcal mol−1) exp. | t 1/2 (ms) | |
| 1a | S | 429 | 515, 552 | 6.2 | 4300 | 13.3 (t) | 15.0 | 18.5 |
| 1b | Se | 446 | 546 | 16.2 | 1800 | 12.8 (t) | 13.8 | 2.3 |
Position of the absorption band (λmax), extinction coefficients for the Z- and E-isomers and quantum yields of forward switching of ITIs 1a and 1b in MeOH. Where possible, experimental λmax,E values are obtained from transient absorption (TA) spectra where two absorption maxima are identified; the most intense absorption is highlighted in bold. Theoretical activation barriers for thermal relaxation were obtained at the M06-2X/6-31+G(d)//6-311++G(2df, 2p) level. The nature of TS is specified in parentheses; t/p stands for twisted/planar structure. Experimental activation energies were calculated with the Eyring equation (with κ = 1). Thermal relaxation rates of ITIs 1a and 1b were recorded in MeOH. Experimental half-lives were obtained from ns TA spectroscopy. Data for 1a have been reported earlier and are reported for comparison.13