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Selected reviews for emissive complexes applied to optical meterials: (a) Amendola, V.; Fabbrizzi, L.; Foti, F.; Licchelli, M.; Mangano, C.; Pallavicini, P.; Poggi, A.; Sacchi, D.; Taglietti, A. Coord. Chem. Rev. 2006, 250, 273.
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Selected review for fundamental study of emissive platinum complexes: (a) Wong, K. M.-C.; Hui, C.-K.; Yu, K.-L.; Yam, V. W.-W. Coord. Chem. Rev. 2002, 229, 123.
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44349169779
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0, the dihedral angle d(N1-N4-N3-N2) is 168.4°, indicating that these atoms are not on one plane, strictly speaking. However, the deviation from the plane is small.
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0, the dihedral angle d(N1-N4-N3-N2) is 168.4°, indicating that these atoms are not on one plane, strictly speaking. However, the deviation from the plane is small.
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44349095509
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1a) were optimized with the DFT(B3PW91)/basis-I method.
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1a) were optimized with the DFT(B3PW91)/basis-I method.
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32
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44349106236
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The activation barrier corresponds to the energy difference between the T1-optimized geometry at r(Pt-Pt, 3.000 Å and the T1-local minimum geometry (1T1b) in 1 and between the T1-optimized geometry at r(Pt-Pt, 3.100 Å and the T1-local minimum geometry (2T1b) in 2, where the transition state is at r(Pt-Pt, 3.000 Å in 1 and at r(Pt-Pt, 3.100 Å in 2. These energy differences were calculated with the DFT(B3PW91)/basis-II//DFT(B3PW91)/basis-I method, where the geometries were optimized at each Pt-Pt distance. These activation barriers are a little bit overestimated, as follows: Because the transition state here is a crossing point of two states, the transition state should be calculated with a multireference method. However, the values presented here are not very much different from the correct values because the PEC of the T
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1 state is not steep but rather flat in the righthand side of the transition state (see Figure 4).
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33
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44349131856
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1b were calculated with the DFT(B3PW91)/basis-II method. (2) The zero-point energy was evaluated with the DFT(B3PW91)/basis-I method. (3) A thermal correction at 298 K was made with the partition function of the vibration movements, in which the partition function was evaluated by the DFT(B3PW91)/basis-I method.
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1b were calculated with the DFT(B3PW91)/basis-II method. (2) The zero-point energy was evaluated with the DFT(B3PW91)/basis-I method. (3) A thermal correction at 298 K was made with the partition function of the vibration movements, in which the partition function was evaluated by the DFT(B3PW91)/basis-I method.
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