Supporting Information
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1 Supporting Information 1,3,5-Triazapentadienes by Nucleophilic Addition to 1,3- and 1,4-Dinitriles - Sterically Constrained Examples by Incorporation into Cyclic Peripheries: Synthesis, Aggregation and Photophysical Properties Agnes Johanna Wrobel, Ralph Lucchesi, Birgit Wibbeling, Constantin- Gabriel Daniliuc, Roland Fröhlich, Ernst-Ulrich Würthwein* Organisch-Chemisches Institut der Universität Münster, Corrensstrasse 40, D Münster, Germany S1
2 Table of contents 1. X-Ray Crystal Structure Analyses S3 2. Experimental Absorption and Emission Spectra with calculated Absorption Spectra for comparison (see also below) S H and 13 C NMR Spectra S20 4. Quantum Chemical Calculations S38 a) M062x/ G(d,p) + GD3 Geometry Optimizations S38 b) TD-CAM-B3LYP/6-311+G(d,p) - Geometry Optimizations S52 c) Calculated Excitations (only the 10 longest wavelength excitations are shown) S61 d) Orbitalplots (TD-CAM-B3LYP/6-311+G(d,p) with orbital numbering and energies (ev) S76 S2
3 X-Ray Crystal Structure Analyses X-Ray diffraction: Data sets were collected with a Nonius KappaCCD diffractometer. Programs used: data collection, COLLECT (R. W. W. Hooft, Bruker AXS, 2008, Delft, The Netherlands); data reduction Denzo-SMN (Z. Otwinowski, W. Minor, Methods Enzymol. 1997, 276, ); absorption correction, Denzo (Z. Otwinowski, D. Borek, W. Majewski, W. Minor, Acta Crystallogr. 2003, A59, ); structure solution SHELXS-97 (G. M. Sheldrick, Acta Crystallogr. 1990, A46, ); structure refinement SHELXL-97 (G. M. Sheldrick, Acta Crystallogr. 2008, A64, ) and graphics, XP (BrukerAXS, 2000) and Schakal 97 (E. Keller, Freiburg). R-values are given for observed reflections, and wr 2 values are given for all reflections. Exceptions and special features: One disordered over two positions acetone molecule was found in the asymmetrical unit of compound 11c. Several restraints (SADI, SAME, ISOR and SIMU) were used in order to improve refinement stability. For compound 12c a partial disordered five membered ring over two positions was found in the asymmetrical unit. Several restraints (SADI, SAME, ISOR and SIMU) were used in order to improve refinement stability. X-ray crystal structure analysis of 8: formula C 14 H 8 N 2, M = , pale yellow crystal, 0.25 x 0.10 x 0.08 mm, a = (4), b = (1), c = (4) Å, β = (1), V = (1) Å 3, ρ calc = gcm -3, μ = mm -1, empirical absorption correction (0.861 T 0.952), Z = 4, monoclinic, space group C2/c (No. 15), λ = Å, T = 223(2) K, ω and φ scans, 2543 reflections collected (±h, ±k, ±l), [(sin )/λ] = 0.60 Å -1, 857 independent (R int = 0.033) and 746 observed reflections [I>2σ(I)], 73 refined parameters, R = 0.042, wr 2 = 0.115, max. (min.) residual electron density 0.10 (-0.13) e.å -3, hydrogen atoms calculated and refined as riding atoms. Figure S1. ORTEP diagram of 8 with ellipsoids shown at the 30% probability level. S3
4 X-ray crystal structure analysis of 10a: formula C 18 H 13 N 3, M = , red crystal, 0.25 x 0.20 x 0.15 mm, a = (3), b = (1), c = (5) Å, β = (1), V = (1) Å 3, ρ calc = gcm -3, μ = mm -1, empirical absorption correction (0.979 T 0.987), Z = 4, monoclinic, space group P2 1 /n (No. 14), λ = Å, T = 223(2) K, ω and φ scans, reflections collected (±h, ±k, ±l), [(sin )/λ] = 0.60 Å -1, 2664 independent (R int = 0.050) and 1938 observed reflections [I>2σ(I)], 198 refined parameters, R = 0.045, wr 2 = 0.126, max. (min.) residual electron density 0.16 (-0.21) e.å -3, the hydrogen atoms at N2 were refined freely; others were calculated and refined as riding atoms. Figure S2. ORTEP diagram of 10a with ellipsoids shown at the 30% probability level. S4
5 X-ray crystal structure analysis of 10b: formula C 19 H 15 N 3, M = , yellow crystal, 0.35 x 0.05 x 0.03 mm, a = (4), b = (8), c = (16) Å, β = (3), V = (2) Å 3, ρ calc = gcm -3, μ = mm -1, empirical absorption correction (0.814 T 0.981), Z = 4, monoclinic, space group P2 1 /c (No. 14), λ = Å, T = 223(2) K, ω and φ scans, 9119 reflections collected (±h, ±k, ±l), [(sin )/λ] = 0.60 Å -1, 2460 independent (R int = 0.066) and 1610 observed reflections [I>2σ(I)], 208 refined parameters, R = 0.053, wr 2 = 0.148, max. (min.) residual electron density 0.16 (-0.16) e.å -3, the hydrogen atoms at N2 were refined freely, but with N-H distance restraint (SADI); others were calculated and refined as riding atoms. Figure S3. ORTEP diagram of 10b with ellipsoids shown at the 30% probability level. S5
6 X-ray crystal structure analysis of 10c: formula C 17 H 12 N 4, M = , yellow crystal, 0.25 x 0.10 x 0.07 mm, a = (1), b = (1), c = (1) Å, β = (1), V = (1) Å 3, ρ calc = gcm -3, μ = mm -1, empirical absorption correction (0.846 T 0.953), Z = 4, monoclinic, space group P2 1 /c (No. 14), λ = Å, T = 223(2) K, ω and φ scans, 8735 reflections collected (±h, ±k, ±l), [(sin )/λ] = 0.60 Å -1, 2213 independent (R int = 0.049) and 1744 observed reflections [I>2σ(I)], 198 refined parameters, R = 0.042, wr 2 = 0.120, max. (min.) residual electron density 0.14 (-0.16) e.å -3, the hydrogen atoms at N1 and N2 were refined freely; others were calculated and refined as riding atoms. Figure S4. ORTEP diagram of 10c with ellipsoids shown at the 30% probability level. S6
7 X-ray crystal structure analysis of 11b: formula C 19 H 14 N 4 ٠ H 2 O, M = , colourless crystal, 0.20 x 0.12 x 0.03 mm, a = (5), b = (2), c = (6) Å, β = (1), V = (2) Å 3, ρ calc = gcm -3, μ = mm -1, empirical absorption correction (0.983 T 0.997), Z = 8, monoclinic, space group C2/c (No. 15), λ = Å, T = 223(2) K, ω and φ scans, reflections collected (±h, ±k, ±l), [(sin )/λ] = 0.60 Å -1, 3250 independent (R int = 0.078) and 2299 observed reflections [I>2σ(I)], 233 refined parameters, R = 0.063, wr 2 = 0.152, max. (min.) residual electron density 0.22 (-0.20) e.å -3, the hydrogen atoms at O1 and N2 were refined freely; others were calculated and refined as riding atoms. Figure S5. ORTEP diagram of 11b with ellipsoids shown at the 30% probability level. S7
8 X-ray crystal structure analysis of 11c: formula C 16 H 16 N 4 ٠ 0.5 x C 3 H 6 O, M = , colourless crystal, 0.25 x 0.12 x 0.07 mm, a = (7), b = (4), c = (7) Å, β = (3), V = (2) Å 3, ρ calc = gcm -3, μ = mm -1, empirical absorption correction (0.865 T 0.959), Z = 8, monoclinic, space group Cc (No. 9), λ = Å, T = 223(2) K, ω and φ scans, reflections collected (±h, ±k, ±l), [(sin )/λ] = 0.60 Å -1, 5061 independent (R int = 0.040) and 4829 observed reflections [I>2σ(I)], 456 refined parameters, R = 0.038, wr 2 = 0.097, max. (min.) residual electron density 0.40 (-0.12) e.å -3, the hydrogen atoms at N2A and N2B were refined freely; others were calculated and refined as riding atoms. Figure S6. ORTEP diagram of 11c with ellipsoids shown at the 30% probability level. S8
9 X-ray crystal structure analysis of 12a: formula C 20 H 23 N 3, M = , yellow crystal, 0.35 x 0.15 x 0.08 mm, a = (1), b = (1), c = (1) Å, β = (1), V = (2) Å 3, ρ calc = gcm -3, μ = mm -1, empirical absorption correction (0.833 T 0.958), Z = 4, monoclinic, space group P2 1 /n (No. 14), λ = Å, T = 223(2) K, ω and φ scans, reflections collected (±h, ±k, ±l), [(sin )/λ] = 0.60 Å -1, 3030 independent (R int = 0.039) and 2749 observed reflections [I>2σ(I)], 219 refined parameters, R = 0.044, wr 2 = 0.115, max. (min.) residual electron density 0.22 (-0.19) e.å -3, the hydrogen atoms at N2 were refined freely; others were calculated and refined as riding atoms. Figure S7. ORTEP diagram of 12a with ellipsoids shown at the 30% probability level. S9
10 X-ray crystal structure analysis of 12b: formula C 15 H 22 N 4, M = , colourless crystal, 0.20 x 0.10 x 0.07 mm, a = (9), b = (5), c = (8) Å, β = (5), V = (3) Å 3, ρ calc = gcm -3, μ = mm -1, empirical absorption correction (0.897 T 0.962), Z = 8, monoclinic, space group C2/c (No. 15), λ = Å, T = 223(2) K, ω and φ scans, reflections collected (±h, ±k, ±l), [(sin )/λ] = 0.60 Å -1, 2598 independent (R int = 0.047) and 2205 observed reflections [I>2σ(I)], 185 refined parameters, R = 0.042, wr 2 = 0.116, max. (min.) residual electron density 0.14 (-0.13) e.å -3, the hydrogen atoms at N2 were refined freely; others were calculated and refined as riding atoms. Figure S8. ORTEP diagram of 12b with ellipsoids shown at the 30% probability level. S10
11 X-ray crystal structure analysis of 12c: formula C 20 H 21 N 3 ٠ 2 x 0.5 C 7 H 8, M = , pale yellow crystal, 0.40 x 0.15 x 0.12 mm, a = (5), b = (5), c = (8) Å, α = (2), β = (2), γ = (2), V = (1) Å 3, ρ calc = gcm -3, μ = mm -1, empirical absorption correction (0.947 T 0.977), Z = 2, triclinic, space group P1 (No. 2), λ = Å, T = 223(2) K, ω and φ scans, reflections collected (±h, ±k, ±l), [(sin )/λ] = 0.60 Å -1, 3817 independent (R int = 0.041) and 3281 observed reflections [I>2σ(I)], 331 refined parameters, R = 0.053, wr 2 = 0.149, max. (min.) residual electron density 0.27 (- 0.24) e.å -3, the hydrogen atoms at N2 were refined freely, but with N-H distance restraint (SADI); others were calculated and refined as riding atoms. Figure S9. ORTEP diagram of 12c with ellipsoids shown at the 30% probability level. S11
12 X-ray crystal structure analysis of 12d: formula C 20 H 22 N 4, M = , yellow crystal, 0.30 x 0.30 x 0.10 mm, a = (4), b = (2), c = (6) Å, β = (1), V = (2) Å 3, ρ calc = gcm -3, μ = mm -1, empirical absorption correction (0.977 T 0.992), Z = 8, monoclinic, space group C2/c (No. 15), λ = Å, T = 223(2) K, ω and φ scans, 7944 reflections collected (±h, ±k, ±l), [(sin )/λ] = 0.60 Å -1, 2836 independent (R int = 0.041) and 2543 observed reflections [I>2σ(I)], 226 refined parameters, R = 0.051, wr 2 = 0.125, max. (min.) residual electron density 0.14 (-0.14) e.å -3, the hydrogen atoms at N2 were refined freely; others were calculated and refined as riding atoms. Figure S10. ORTEP diagram of 12d with ellipsoids shown at the 30% probability level. S12
13 X-ray crystal structure analysis of 12e: formula C 18 H 18 N 4 ٠ C 3 H 6 O, M = , pale yellow crystal, 0.20 x 0.20 x 0.15 mm, a = (6), b = (4), c = (7) Å, β = (2), V = (2) Å 3, ρ calc = gcm -3, μ = mm -1, empirical absorption correction (0.888 T 0.914), Z = 4, monoclinic, space group P2 1 /c (No. 14), λ = Å, T = 223(2) K, ω and φ scans, reflections collected (±h, ±k, ±l), [(sin )/λ] = 0.60 Å -1, 3369 independent (R int = 0.040) and 2990 observed reflections [I>2σ(I)], 245 refined parameters, R = 0.047, wr 2 = 0.129, max. (min.) residual electron density 0.31 (-0.20) e.å -3, the hydrogen atoms at N2 were refined freely; others were calculated and refined as riding atoms. Figure S11. ORTEP diagram of 12e with ellipsoids shown at the 30% probability level. S13
14 X-ray crystal structure analysis of 12f: formula C 17 H 23 N 3, M = , yellow crystal, 0.50 x 0.40 x 0.20 mm, a = (1), b = (1), c = (2) Å, α = (1), β = (1), γ = (1), V = 730.3(2) Å 3, ρ calc = gcm -3, μ = mm -1, empirical absorption correction (0.765 T 0.895), Z = 2, triclinic, space group P 1 (No. 2), λ = Å, T = 223(2) K, ω and φ scans, 8996 reflections collected (±h, ±k, ±l), [(sin )/λ] = 0.60 Å -1, 2546 independent (R int = 0.033) and 2422 observed reflections [I>2σ(I)], 187 refined parameters, R = 0.041, wr 2 = 0.106, max. (min.) residual electron density 0.19 (-0.16) e.å -3, the hydrogen atoms at N2 were refined freely; others were calculated and refined as riding atoms. Figure S12. ORTEP diagram of 12f with ellipsoids shown at the 30% probability level. S14
15 X-ray crystal structure analysis of 13: formula C 13 H 14 N 2 O, M = , colourless crystal, 0.35 x 0.25 x 0.03 mm, a = (4), b = (3), c = (2) Å, β = (1), V = (1) Å 3, ρ calc = gcm -3, μ = mm -1, empirical absorption correction (0.971 T 0.997), Z = 8, monoclinic, space group C2/c (No. 15), λ = Å, T = 223(2) K, ω and φ scans, reflections collected (±h, ±k, ±l), [(sin )/λ] = 0.60 Å -1, 2540 independent (R int = 0.055) and 1961 observed reflections [I>2σ(I)], 157 refined parameters, R = 0.060, wr 2 = 0.139, max. (min.) residual electron density 0.24 (-0.17) e.å -3, the hydrogen atoms at N2 were refined freely; others were calculated and refined as riding atoms. Figure S13. ORTEP diagram of 13 with ellipsoids shown at the 30% probability level. S15
16 Experimental Absorption and Emission Spectra with calculated Absorption Spectra for comparison (see also pages S60 ff) Norm. Absorption / Norm. Emission 1,0 0,8 0,6 0,4 0,2 0, Wavelength (nm) Figure S14. Experimental UV/Vis- and fluorescence spectrum of 10a. Monomer Dimer Figure S15. Calculated UV/Vis spectra for the monomer (top) and the dimer (bottom) of 10a. S16
17 Figure S16. Experimental UV/Vis- and fluorescence spectrum of 10b. Monomer Dimer Figure S17. Calculated UV/Vis spectra for the monomer (top) and the dimer (bottom) of 10b. S17
18 Figure S18. Experimental UV/Vis- and fluorescence spectrum of 10c. Figure S19. Calculated UV/Vis spectrum of 10c. S18
19 Figure S20. Experimental UV/Vis- and fluorescence spectrum of 12d. Monomer Dimer Figure S21. Calculated UV/Vis spectra for the monomer (top) and the dimer (bottom) of 12d. S19
20 1 H and 13 C NMR Spectra 7 Figure S22: 1 H (Top; 300 MHz) in d 6 -DMSO and 13 C { 1 H} NMR (bottom, 100 MHz) spectra of compound 7 in CDCl 3. S20
21 9a Figure S23: 1 H (Top; 400 MHz) and 13 C { 1 H} NMR (bottom, 100 MHz) spectra of compound 9a in CDCl 3. S21
22 9b Figure S24: 1 H (Top; 300 MHz) and 13 C { 1 H} NMR (bottom, 75 MHz) spectra of compound 9b in CDCl 3. S22
23 10a Figure S25: 1 H (Top; 300 MHz) and 13 C { 1 H} NMR (bottom, 75 MHz) spectra of compound 10a in d 6 -DMSO. S23
24 10b Figure S26: 1 H (Top; 300 MHz) and 13 C { 1 H} NMR (bottom, 75 MHz) spectra of compound 10b in d 6 -DMSO. S24
25 10c Figure S27: 1 H (Top; 400 MHz) and 13 C { 1 H} NMR (bottom, 100 MHz) spectra of compound 10c in d 6 -DMSO. S25
26 10d Figure S28: 1 H (Top; 300 MHz) and 13 C { 1 H} NMR (bottom, 75 MHz) spectra of compound 10d in CDCl 3 (The compound is quite sensitive, showing impurities in the spectra). S26
27 10e Figure S29: 1 H (Top; 300 MHz) and 13 C { 1 H} NMR (bottom, 75 MHz) spectra of compound 10e in d 6 -DMSO 3. S27
28 11a Figure S30: 1 H (Top; 300 MHz) and 13 C { 1 H} NMR (bottom, 75 MHz) spectra of compound 11a in d 6 -DMSO. S28
29 11b Figure S31: 1 H (Top; 300 MHz) and 13 C { 1 H} NMR (bottom, 75 MHz) spectra of compound 11b in d 6 -DMSO. S29
30 11c Figure S32: 1 H (Top; 300 MHz) and 13 C { 1 H} NMR (bottom, 75 MHz) spectra of compound 11c in CDCl 3. S30
31 12a Figure S33: 1 H (Top; 400 MHz) and 13 C { 1 H} NMR (bottom, 150 MHz) spectra of compound 12a in CDCl 3. S31
32 12b Figure S34: 1 H (Top; 400 MHz) and 13 C { 1 H} NMR (bottom, 100 MHz) spectra of compound 12b in CDCl 3. S32
33 12c Figure S35: 1 H (Top; 400 MHz) and 13 C { 1 H} NMR (bottom, 100 MHz) spectra of compound 12c in d 6 -DMSO. S33
34 12d Figure S36: 1 H (Top; 400 MHz) and 13 C { 1 H} NMR (bottom, 100 MHz) spectra of compound 12d in CDCl 3. S34
35 12e Figure S37: 1 H (Top; 400 MHz) and 13 C { 1 H} NMR (bottom, 100 MHz) spectra of compound 12e in CDCl 3. S35
36 12f Figure S38: 1 H (Top; 300 MHz) and 13 C { 1 H} NMR (bottom, 75 MHz) spectra of compound 12f in CDCl 3. S36
37 14 Figure S39: 1 H (Top; 300 MHz) and 13 C { 1 H} NMR (bottom, 75 MHz) spectra of compound 14 in d 6 -DMSO. S37
38 Quantum Chemical Calculations 1,2,3 Results from Gaussian09-Outputs (Coordinates, Total energies (a.u.), Number of imaginary frequencies) a) M062x/ G(d,p) + GD3 Geometry Optimizations 2-(1-Cyano-cyclopentyl)-benzonitrile 9b E tot = a.u. (0) Element x y z NBO-Charge (benzylic) (aromatic) Z-2-Aminopyridine anion E tot = a.u. (0) Element x y z NBO-Charge (pyridyl) S38
39 7 (amine) Aniline-anion E tot = a.u. (0) Element x y z NBO-Charge b-monomer E tot = a.u. (0) S39
40 b-dimer E tot = a.u. (0) S40
41 c-monomer E tot = a.u. (0) S41
42 c-monomer-TS E tot = a.u. (1) S42
43 c-dimer E tot = a.u. (0) S43
44 b-monomer E tot = a.u. (0) S44
45 b-dimer E tot = a.u. (0) S45
46 S46
47 d-monomer E tot = a.u. (0) S47
48 d-dimer E tot = a.u. (0) S48
49 S49
50 monomer E tot = a.u. (0) dimer E tot = a.u. (0) S50
51 S51
52 b) TD-CAM-B3LYP/6-311+G(d,p) Geometry Optimizations 10a Monomer: E(RCAM-B3LYP) = au S52
53 a-Dimer: E(RCAM-B3LYP) = au S53
54 b-Monomer: E(RCAM-B3LYP) = au S54
55 b-Dimer: E(RCAM-B3LYP) = = au S55
56 c (Monomer): E(RCAM-B3LYP) = au S56
57 d-Monomer: E(RCAM-B3LYP) = au S57
58 d-Dimer: E(RCAM-B3LYP) = au S58
59 S59
60 S60
61 c) Calculated Excitations (only the 10 longest wavelength excitations are shown) 10a Monomer (solid) and Dimer (dashed) Calculated extinction Wavelength (nm) 10a-Monomer Excitation energies and oscillator strengths: Excited State 1: Singlet-A ev nm f= > This state for optimization and/or second-order correction. Total Energy, E(TD-HF/TD-KS) = Copying the excited state density for this state as the 1-particle RhoCI density. Excited State 2: Singlet-A ev nm f= > > Excited State 3: Singlet-A ev nm f= > > > > > S61
62 Excited State 4: Singlet-A ev nm f= > > > > > > Excited State 5: Singlet-A ev nm f= > > > > > > Excited State 6: Singlet-A ev nm f= > > > > > > > > > > > Excited State 7: Singlet-A ev nm f= > > > > > > > Excited State 8: Singlet-A ev nm f= > > > > > > > > > Excited State 9: Singlet-A ev nm f= > > > > > S62
63 Excited State 10: Singlet-A ev nm f= > > > > > > > a-Dimer Excitation energies and oscillator strengths: Excited State 1: Singlet-A ev nm f= > > This state for optimization and/or second-order correction. Total Energy, E(TD-HF/TD-KS) = Copying the excited state density for this state as the 1-particle RhoCI density. Excited State 2: Singlet-A ev nm f= > > Excited State 3: Singlet-A ev nm f= > > Excited State 4: Singlet-A ev nm f= > > Excited State 5: Singlet-A ev nm f= > > > > > > > > > Excited State 6: Singlet-A ev nm f= > > > > > > > > S63
64 Excited State 7: Singlet-A ev nm f= > > > > > > > > > > Excited State 8: Singlet-A ev nm f= > > > > > Excited State 9: Singlet-A ev nm f= > > > > > > > > > > > > > > > Excited State 10: Singlet-A ev nm f= > > > > > > > > > S64
65 10b Monomer (solid) and Dimer (dashed) 10b-Monomer Excitation energies and oscillator strengths: Excited State 1: Singlet-A ev nm f= > This state for optimization and/or second-order correction. Total Energy, E(TD-HF/TD-KS) = Copying the excited state density for this state as the 1-particle RhoCI density. Excited State 2: Singlet-A ev nm f= > > Excited State 3: Singlet-A ev nm f= > > > > > Excited State 4: Singlet-A ev nm f= > > > > > > S65
66 Excited State 5: Singlet-A ev nm f= > > > > > > > Excited State 6: Singlet-A ev nm f= > > > > > > > > > > > > Excited State 7: Singlet-A ev nm f= > > > > > > > Excited State 8: Singlet-A ev nm f= > > > > > > > > Excited State 9: Singlet-A ev nm f= > > > > > > > Excited State 10: Singlet-A ev nm f= > > > > S66
67 74 -> > > > > b-Dimer Excitation energies and oscillator strengths: Excited State 1: Singlet-A ev nm f= > > This state for optimization and/or second-order correction. Total Energy, E(TD-HF/TD-KS) = Copying the excited state density for this state as the 1-particle RhoCI density. Excited State 2: Singlet-A ev nm f= > > Excited State 3: Singlet-A ev nm f= > > Excited State 4: Singlet-A ev nm f= > > Excited State 5: Singlet-A ev nm f= > > > > > > > Excited State 6: Singlet-A ev nm f= > > > > > > > > > Excited State 7: Singlet-A ev nm f= > > S67
68 147 -> > > Excited State 8: Singlet-A ev nm f= > > > Excited State 9: Singlet-A ev nm f= > > > > > > > > > > > Excited State 10: Singlet-A ev nm f= > > > > > > > > > S68
69 10c-Monomer Excitation energies and oscillator strengths: Excited State 1: Singlet-A ev nm f= > This state for optimization and/or second-order correction. Total Energy, E(TD-HF/TD-KS) = Copying the excited state density for this state as the 1-particle RhoCI density. Excited State 2: Singlet-A ev nm f= > > > Excited State 3: Singlet-A ev nm f= > > > > > Excited State 4: Singlet-A ev nm f= > > > > Excited State 5: Singlet-A ev nm f= > > S69
70 70 -> > > Excited State 6: Singlet-A ev nm f= > > > Excited State 7: Singlet-A ev nm f= > > > > > > Excited State 8: Singlet-A ev nm f= > > > > > Excited State 9: Singlet-A ev nm f= > > > > Excited State 10: Singlet-A ev nm f= > > > > > > S70
71 12d Monomer (solid) and Dimer (dashed) 12d-Monomer Excitation energies and oscillator strengths: Excited State 1: Singlet-A ev nm f= > This state for optimization and/or second-order correction. Total Energy, E(TD-HF/TD-KS) = Copying the excited state density for this state as the 1-particle RhoCI density. Excited State 2: Singlet-A ev nm f= > > > > Excited State 3: Singlet-A ev nm f= > > > > > > Excited State 4: Singlet-A ev nm f= > > > > S71
72 83 -> > > > > > > Excited State 5: Singlet-A ev nm f= > > > > > > > > > Excited State 6: Singlet-A ev nm f= > > > > > > > > > > Excited State 7: Singlet-A ev nm f= > > > > > > > > > > Excited State 8: Singlet-A ev nm f= > > > > > > > > Excited State 9: Singlet-A ev nm f= > > > S72
73 84 -> > > > Excited State 10: Singlet-A ev nm f= > > > > > > > > > > > > > d-Dimer Excitation energies and oscillator strengths: Excited State 1: Singlet-A ev nm f= > > > This state for optimization and/or second-order correction. Total Energy, E(TD-HF/TD-KS) = Copying the excited state density for this state as the 1-particle RhoCI density. Excited State 2: Singlet-A ev nm f= > > > Excited State 3: Singlet-A ev nm f= > > > > > > > > > Excited State 4: Singlet-A ev nm f= > > > > > > > S73
74 170 -> > Excited State 5: Singlet-A ev nm f= > > > > > Excited State 6: Singlet-A ev nm f= > > > > > Excited State 7: Singlet-A ev nm f= > > > > > > > > > > > > > Excited State 8: Singlet-A ev nm f= > > > > > > > > > > > > > Excited State 9: Singlet-A ev nm f= > > > > > > > > > S74
75 170 -> > > Excited State 10: Singlet-A ev nm f= > > > > > > > > > > > S75
76 d) Orbitalplots (TD-CAM-B3LYP/6-311+G(d,p) with orbital numbering and energies (ev)) 10a-Monomer HOMO-1 LUMO+1 70 (HOMO-1) (HOMO) (LUMO) (LUMO+1) S76
77 10a-Dimer HOMO-1 LUMO (HOMO-1) (HOMO) (LUMO) (LUMO+1) S77
78 10b-Monomer HOMO-1 LUMO+1 74 (HOMO-1) (HOMO) (LUMO) (LUMO+1) S78
79 10b-Dimer HOMO-1 LUMO (HOMO-1) (HOMO) (LUMO) (LUMO+1) S79
80 10c-Monomer HOMO-1 LUMO+1 70 (HOMO-1) (HOMO) (LUMO) (LUMO+1) S80
81 12d-Monomer HOMO-1 LUMO+1 84 (HOMO-1) (HOMO) (LUMO) (LUMO+1) S81
82 12d-Dimer HOMO-1 LUMO (HOMO-1) (HOMO) (LUMO) (LUMO+1) S82
Photo-Induced Self-Assembly of Pt(II)-Linked Rings and Cages via the Photolabilization of a Pt(II) Pyridine Bond
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