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. 2019 Jun 3;10:2390. doi: 10.1038/s41467-019-10251-8

Table 1.

Computational studies on solvents on ITI photo-isomerization

Z-isomer
Solvent (εr) λmax,Z (nm) Transition
exp. calc. ππ*/nπ* θ1(C1-C2-N4-C5)/θ2(C2-N4-C5-C6) ΔμES-GS,Z(D)
Cyclohexane (2.02) 416 373

S0→S2

0.61/0.18

179.8/49.8 1.77
Toluene (2.37) 430 374

S0→S2

0.61/0.20

179.8/50.2 1.86
CHCl3 (4.71) 435 378

S0→S2

0.61/0.20

180.0/51.4 2.26
MeOH (32.61) 429 398

S0→S1

0.58/0.34

−179.8/54.1 1.55
DMSO (46.83) 432 379

S0→S2

0.61/0.24

180.0/54.1 2.82
E-isomer
Solvent (εr) λmax,E (nm) Transition
exp. calc. ππ*/nπ* θ1(C1-C2-N4-C5)/θ2(C2-N4-C5-C6) ΔμES-GS,E(D)
Cyclohexane (2.02) 517, 554 520

S0→S1

0.55/0.31

9.5/60.6 −2.85
Toluene (2.37) 510, 551 519

S0→S1

0.55/0.31

9.5/61.7 −2.96
CHCl3 (4.71) 506, 549, 513

S0→S1

0.55/0.31

9.3/62.9 −3.48
MeOH (32.61) 515, 552 505

S0→S1

0.54/0.30

9.3/66.0 −4.17
DMSO (46.83) 514, 553 503

S0→S1

0.55/0.31

9.0/66.9 −4.05
Transition state
Solvent (εr) Δλmax (nm) t1/2 (ms) ΔGZ-E# (kcal/mol)
exp. calc. exp. exp. calc. θ1(C1-C2-N4-C5)/θ2(C2-N4-C5-C6) μGS,TS(D)
Gas phase (1.00) NA (13.2) NA (0.0/0.0) NA (1.20)
Cyclohexane (2.02) 101, 138 147 9.5 ± 0.4 14.1 12.8 (12.8) 0.0/90.4 (−0.1/0.1) 3.85 (1.30)
Toluene (2.37) 80, 121 145 12.4 ± 0.9 14.2 12.7 (12.9) 0.0/90.4 (−0.1/0.1) 3.97 (1.33)
CHCl3 (4.71) 71, 114 135 16.9 ± 1.2 14.4 13.3 (13.7) 0.0/90.4 (−0.1/0.1) 4.44 (1.52)
MeOH (32.61) 86, 123 107 18.5 ± 1.4 14.4 14.4 (NA) 0.0/87.5 (NA) 5.25 (NA)
DMSO (46.83) 82, 121 124 23.3 ± 2.0 14.6 13.5 (NA) 0.0/90.2 (NA) 4.92 (NA)

Solvatochromic shifts of λmax for the Z (Top) and E (Middle) isomers of ITI 1a. Experimental λmax,E values are obtained from TA that show two absorption maxima which are both reported and the maximum, of which the one with the highest absorption is highlighted in bold. Theoretical λmax values and the difference of GS and ES dipole moments (ΔμES-GS) were obtained at the SMD-TD-M06-2X/6-311++G(2df,2p) level using the SMD-M06-2X/6-31+G(d) geometries, from which also twisting angles θ1 and θ2 were derived (see Fig. 2a). Bottom: Thermal relaxation of ITI 1a. Experimental half-lives were calculated from ms TA. The GS dipole moments for the transition state (μGS,TS) were obtained at the SMD-M06-2X/6-31+G(d) level, at which also the twisting angles θ1 and θ2 as well as the activation barriers for thermal relaxation were derived (see Fig. 2a). The data in parentheses refer to a planar TS structure