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

Table 2.

Computational studies on substituent effects on ITI photo-isomerization

Z-isomer
R (Hammet constant σ) λmax,Z (nm) Transition
exp. calc. ππ*/nπ* θ1(C1-C2-N4-C5)/θ2(C2-N4-C5-C6) ΔμES-GS,Z (D) ε (mol−1cm−1)
1a H (0.00) 429 398

S0→S1

0.58/0.38

−179.8/54.1 1.55 4300
1b MeO (−0.27) 448 413

S0→S1

0.62/0.29

−179.1/38.6 4.43 11000
1c Me (−0.17) 434 406

S0→S1

0.61/0.32

−179.9/50.3 2.66 5700
1d COOMe (0.45) 427 399

S0→S1

0.56/−0.15

−179.1/60.8 0.85 2300
1e CF3 (0.54) 424 391

S0→S1

0.54/0.37

−179.1/62.0 −0.62 2100
1 f NO2 (0.78) 390

S0→S1

0.53/−0.33

−178.9/67.3 −0.26 2600
E-isomer
R (Hammet constant σ)  λmax,E (nm) Transition
exp. calc. ππ*/nπ* θ1(C1-C2-N4-C5)/ θ2(C2-N4-C5-C6) ΔμES-GS,E (D)
1a H (0.00) 515, 552 505

S0→S1

0.54/0.30

9.3/66.0 −4.16
1b MeO (−0.27) 553 533

S0→S1

0.58/−0.32

12.4/52.9 2.37
1c Me (−0.17) 511, 548, 519

S0→S1

0.58/−0.31

9.9/63.2 −1.01
1d COOMe (0.45) 503 484

S0→S1

0.52/−0.31

0.26/93.0 −4.45
1e CF3 (0.54) 500 482

S0→S1

0.52/−0.31

2.23/86.1 −5.81
1 f NO2 (0.78) 501 470

S0→S1

0.54/0.30

0.00/−92.9 −5.85
Transition state
R (Hammet constant σ) Δλmax (nm) t1/2 (ms) Ea,E-Z (kcal/mol) α(C2-N4-C5)/ ΔμGS-TS,Z
exp. calc. exp. exp. calc. θ2(C2-N4-C5-C6) (D) φZ-E (%)
1a H (0.00) 86, 123 107 18.5 ± 1.4 14.4 14.4 177.2/87.5 −0.02 6.2
1b MeO (−0.27) 105 120 12.7 ± 0.5 14.2 13.0 177.7/0.0 −2.45 4.5
1c Me (−0.17) 77, 114 113 21.1 ± 1.2 14.5 14.0 177.7/0.0 −2.68 5.4
1d COOMe (0.45) 76 85 4.0 ± 0.3 13.6 13.1 177.6/92.0 0.38 6.3
1e CF3 (0.54) 76 91 9.9 ± 1.0 14.1 13.6 177.6/90.1 0.94 4.9
1 f NO2 (0.78) 80 2.8 ± 0.5 13.4 12.0 177.8/90.1 2.48 4.1

Shifts of λmax for the Z (Top) and E (Middle) isomers of ITIs 1af in MeOH. Experimental λmax,E values are obtained from TA that show two absorption maxima which are both reported with the maximum with the highest absorption 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, Fig. 2a) were derived. Bottom: Thermal relaxation of ITIs 1af in MeOH. Experimental half-lives were calculated from ms TA spectroscopy. The differences of dipole moment of the transition state and that of the Z-form in their GS (ΔμGS-TS,Z) were obtained at the SMD-M06-2X/6-31+G(d) level, at which also the transition state twisting angles (θ1 and θ2) as well as the activation barriers for thermal relaxation were derived