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Schmidt, M. W.; Baldridge, K. K.; Boatz, J. A.; Elbert, S. T.; Gordon, M. S.; Jensen, J. J.; Koseki, S.; Matsunaga, N.; Nguyen, K. A.; Su, S.; Windus, T. L.; Dupuis, M.; Montgomery, J. A. J. Comput. Chem. 1993, 14, 1347.
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Schmidt, M.W.1
Baldridge, K.K.2
Boatz, J.A.3
Elbert, S.T.4
Gordon, M.S.5
Jensen, J.J.6
Koseki, S.7
Matsunaga, N.8
Nguyen, K.A.9
Su, S.10
Windus, T.L.11
Dupuis, M.12
Montgomery, J.A.13
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94
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20944439093
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note
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The variations in the vertical electron affinity of the dioxetanone and dioxetane functionalities as a function of the O-O bond distance are summarized in Figure S6 (Supporting Information).
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95
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0344425248
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Schmidt, S. P.; Vincent, M. A.; Dykstra, C. E.; Schuster, G. B. J. Am. Chem. Soc. 1981, 103, 1292.
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Schmidt, S.P.1
Vincent, M.A.2
Dykstra, C.E.3
Schuster, G.B.4
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98
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0014575021
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(b) McElroy, W. D.; Seliger, H. H.; White, E. H. Photochem. Photobiol. 1969, 10, 153.
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Photochem. Photobiol.
, vol.10
, pp. 153
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McElroy, W.D.1
Seliger, H.H.2
White, E.H.3
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99
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0001424344
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(c) White, E. H.; Steinmetz, M. G.; Miano, J. D.; Wildes, P. D.; Moreland, R. J. Am. Chem. Soc. 1980, 102, 3199.
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J. Am. Chem. Soc.
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White, E.H.1
Steinmetz, M.G.2
Miano, J.D.3
Wildes, P.D.4
Moreland, R.5
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101
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0037905684
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Orlova, G.; Goddard, J. D.; Brovko, L. Y. J. Am. Chem. Soc. 2003, 125, 6962.
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Orlova, G.1
Goddard, J.D.2
Brovko, L.Y.3
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102
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20944445555
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note
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-1. In contrast, the addition of a phenoxide-anion group gives rise to the CT process, which corresponds to the nonstepwise mechanism; that is, no intermediate is formed.
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105
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20944451725
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note
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The results of the IRC analysis for para-1c are given in Figure S8 (Supporting Information).
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107
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0042387908
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(b) Silva, S. M.; Wagner, K.; Weiss, D.; Beckert, R.; Stevani, C. V.; Baader, W. J. Luminescence 2002, 17, 362.
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(2002)
Luminescence
, vol.17
, pp. 362
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Silva, S.M.1
Wagner, K.2
Weiss, D.3
Beckert, R.4
Stevani, C.V.5
Baader, W.J.6
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109
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20944450681
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note
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2 moiety.
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110
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20944446716
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note
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1 states of para-1c and meta-1c calculated by the B3LYP method are shown in Figure S9 (Supporting Information).
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111
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20944440860
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33d however, the HF method tends to overestimate the diradical character (yHOMO > 90%) for the back CT region, characterized by the B 3LYP method, and provides biased results in favor of diradical pathway (see Figure S2). Therefore, the calculations for the back CT region as well as the CT TSs were conducted using the B3LYP method.
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112
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20944432497
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note
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-1.
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113
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20944441099
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note
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We also tried to locate the equilibrium structures (min.) and the CT TSs of para- and meta-1c in benzene and DMSO at the PCM (for min.) or Onsager model (for CT TSs) B3LYP/6-31+G(d) levels. It was found that, despite the presence of the solvent reaction field, there are insignificant changes in the equilibrium geometries; however, the relatively large structural change of the CT TS on going from the gas phase to a solution is made explicit in the O-O distance and is largely dependent on the degree of solvent polarity. The detailed results are summarized in Table S3 (Supporting Information).
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114
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20944435117
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15a
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116
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20944448146
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note
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-1] of the methyl meta-oxybenzoate anion at the PCM HF/6-3I+G(d)//B3LYP/6-31+G(d) level.
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