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19
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58149158814
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2 have been recorded in frozen MeTHF at 80 K and in dichloromethane at room T, and have been taken from ref 6. The absorption and emission spectra of 4T have been recorded in tetradecane at 12 and 290 K.
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2 have been recorded in frozen MeTHF at 80 K and in dichloromethane at room T, and have been taken from ref 6. The absorption and emission spectra of 4T have been recorded in tetradecane at 12 and 290 K.
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20
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4243539377
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TURBOMOLE 5.7.1 quantum-chemical package: Electronic Structure Calculations on Workstation Computers: The Program System TUR- BOMOLE. Ahlrichs, R.; Bär, M.; Häser, M.; Horn, H.; Kölmel. C. Chem. Phys. Lett. 1989, 162, 165.
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TURBOMOLE 5.7.1 quantum-chemical package: Electronic Structure Calculations on Workstation Computers: The Program System TUR- BOMOLE. Ahlrichs, R.; Bär, M.; Häser, M.; Horn, H.; Kölmel. C. Chem. Phys. Lett. 1989, 162, 165.
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21
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0346843091
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Reimers, J.R.1
Cai, Z.-L.2
Bilic, A.3
Hush, N.S.4
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22
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0034801551
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Sluch, M. I.; Godt, A.; Bunz. U. H.; Berg, M. A. J. Am. Chem. Soc. 2001, 123, 6447.
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Sluch, M.I.1
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25
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0034511486
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Karabunarliev, S.1
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Müllen, K.4
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29
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58149152090
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The general recursion formula for displaced distorted harmonic oscillators reads as given in: Henry, B. R.; Siebrand, W. In Organic Molecular Photophxsics; Bilks, J. B., Ed.; John Wiley & Sons Ltd.: Bristol, U.K., 1973; p 218.
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The general recursion formula for displaced distorted harmonic oscillators reads as given in: Henry, B. R.; Siebrand, W. In Organic Molecular Photophxsics; Bilks, J. B., Ed.; John Wiley & Sons Ltd.: Bristol, U.K., 1973; p 218.
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30
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0001024508
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Acta Physicochem
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Duschinsky, F. Acta Physicochem. URSS 1937, 7, 551.
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(1937)
URSS
, vol.7
, pp. 551
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Duschinsky, F.1
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31
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58149148900
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In the case of 4T, the torsional frequencies of the ground state were taken from a non-planar C2 equilibrium geometry because the torsional frequencies of the planar structure were found to be non-real as a result of performing the calculations in vacuo. The suitability of the frequencies of the C2 conformer arises from the almost identical geometries of both structures, and the small dihedral angles between the thiophene rings in the C2 conformer 15-20°
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2 conformer (15-20°).
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32
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76249128064
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DOI:10.1039/B810915J
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Macchi, G.; Milián Medina, B.; Zambianchi, M.; Tubino, R.; Cornil, J.; Barbarella, G.; Gierschner, J.; Meinardi, F. Phys. Chem. Chem. Phys. 2008, DOI:10.1039/B810915J.
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(2008)
Phys. Chem. Chem. Phys
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Macchi, G.1
Milián Medina, B.2
Zambianchi, M.3
Tubino, R.4
Cornil, J.5
Barbarella, G.6
Gierschner, J.7
Meinardi, F.8
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33
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58149171072
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The MOshavebeen depicted using the MOLEKEL4.3 program: Flükiger, P.; Lüthi, H. P.; Portmann, S.; Weber, J. Swiss Center for Scientific Computing, Manno, Switzerland, 2000-2002. Portmann, Stefan; Lüthi, Hans Peter. MOLEKEL: An Interactive Molecular Graphics Tool. CHIMIA 2000, 54, 766.
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The MOshavebeen depicted using the MOLEKEL4.3 program: Flükiger, P.; Lüthi, H. P.; Portmann, S.; Weber, J. Swiss Center for Scientific Computing, Manno, Switzerland, 2000-2002. Portmann, Stefan; Lüthi, Hans Peter. MOLEKEL: An Interactive Molecular Graphics Tool. CHIMIA 2000, 54, 766.
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34
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58149150616
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3b'4 with an average of 2.96 Å. The somewhat longer S• O distances (ca. 3.06 Å) in mixed thiophene-EDOT compounds (ref 3b) arise mainly from the fact that the structures are not planar but show torsional dihedral angles of about 14°.
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3b'4 with an average of 2.96 Å. The somewhat longer S• O distances (ca. 3.06 Å) in mixed thiophene-EDOT compounds (ref 3b) arise mainly from the fact that the structures are not planar but show torsional dihedral angles of about 14°.
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35
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0442279530
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Raos. G.; Famulari, A.: Meille. S. V.; Gallazzi, M. C.; Allegra. G. J. Phys. Chem. A 2004, 108, 691.
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(2004)
J. Phys. Chem. A
, vol.108
, pp. 691
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Raos, G.1
Famulari, A.2
Meille, S.V.3
Gallazzi, M.C.4
Allegra, G.5
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36
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58149157117
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For 2EDOT model calculation at the BHLYP/cc-pVTZ level gives α, 124.02°. β, 121.93° for TP and α, 124.00°. β, 121.94° for 90°. Δ, 0.03. For 2T. α, 123.15°, β, 123.36° for TP and α, 122.53. β, 124.11° for 90°, Δ, 1.37 is obtained
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For 2EDOT model calculation at the BHLYP/cc-pVTZ level gives α = 124.02°. β = 121.93° for TP and α = 124.00°. β = 121.94° for 90°. Δ =-0.03. For 2T. α = 123.15°, β = 123.36° for TP and α = 122.53. β = 124.11° for 90°, Δ =-1.37 is obtained.
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37
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58149165892
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This attractive force can vary significantly; e.g, Raos et al. 29 calculated A, 0.60 for dimethoxy-substituted 2T
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29 calculated A = +0.60 for dimethoxy-substituted 2T.
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38
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58149168010
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2h) yields 2.92 Å, not much smaller than the van der Waals distance (3.05 Å).
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2h) yields 2.92 Å, not much smaller than the van der Waals distance (3.05 Å).
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