Handbook of Aggregation-Induced Emission, Volume 1. Группа авторов

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Handbook of Aggregation-Induced Emission, Volume 1 - Группа авторов


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2.4d, the major differences in the reorganization energies between the gas phase and the solid state are related to the low‐frequency eight‐member annulene flipping vibrational mode. Thus, the fluorescence of COTh upon aggregation is induced by the suppression of the nonradiative decay channel contributed by the electron–vibration coupling between the transition electron and low‐frequency flipping vibration (see Figure 2.2e).

k r (s−1) k ic (s−1) Φ F (%) k r (s−1) k ic (s−1) Φ F (%)
In isolated state In solid phase
TPA [41] 3.34 × 104 4.97 × 107 0.067 3.43 × 107 5.15 × 106 86.95
(CAACAd)CuCl [42] 6.26 × 105 8.38 × 107 0.44 7.83 × 105 1.47 × 104 98.0
COTh [43] 9.80 × 104 4.13 × 109 0.002 6.05 × 105 1.87 × 107 3.13

      2.3.5 Twisting Vibration of Molecular Skeletons

S0 S1 ∣∆(S0 − S1)∣ S0 S1 ∣∆(S0 − S1)∣ Crystal
In gas phase In solid phase
Θ I–II 44.93 22.11 22.82 43.84 31.06 12.78 42.85
Θ II–III −48.58 −24.36 24.22 −48.67 −35.71 12.96 −48.83
Θ III–IV 44.92 22.11 22.81 45.24 32.60 12.64 45.16
Θ I–IV −48.59 −24.36 24.23 −48.94 −35.72 13.22 −46.99

      THBDBA contains two pairs of phenyl rings that are covalently linked through a singly bonded ethyl chain (Figure 2.3); it is almost nonemissive when fully solvated in the THF solution and starts to emit with the addition of water [9]. In THBDBA crystal, each set of phenyl rings locked by the ethyl chain adopts a V‐shaped or “boat” conformation. Theoretical calculation indicates that the single molecule has a λtotal of 6898.6 cm−1, whereas the molecule in a cluster only has 5901.5 cm−1. The normal mode analysis shows that low‐frequency vibrational modes mainly contribute to λtotal for both single molecule and in crystal, but λtotal in the crystal is largely reduced. Upon aggregation, the restriction of low‐frequency twisting motion blocks the nonradiative decay channel and turns the fluorescence on (Figure 2.2g) [9].

      As shown in Section 8.3, the theoretical calculation is an effective tool for unraveling the deep insights into experimental phenomenon; we know that the reorganization energy and DRE play important roles in the AIE mechanism; however, how to validate the theoretically proposed AIE mechanism and visualize the calculated parameters in experiments? In this section, we will bridge the calculated parameters and the experimental measurable parameters to validate our above


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