Helicenes are promising candidates for chiral optoelectronic materials because of their helically twisted π-conjugated system. However, the emission intensity of unsubstituted helicenes is very weak (Φf < 0.05) due to a small oscillator strength for the S₁ → S₀ transition. In this work, we investigated the substitution position of the [7]helicene framework so that the S₁ → S₀ transition has a large transition magnetic dipole moment (TMDM) and is partially symmetry-allowed. A [7]helicene derivative thus designed showed a large fluorescence emission rate (kf = 0.02 ns⁻¹) and a large TMDM for the S₁ → S₀ transition (|m| = 2.37 × 10⁻²⁰ erg·Gauss⁻¹), which are more than 10 times greater than those of unsubstituted [7]helicene (kf = 0.001 ns⁻¹, |m| = 0.045 × 10⁻²⁰ erg·Gauss⁻¹). As a result, we achieved the [7]helicene derivative whose dissymmetry factor of CPL and fluorescence quantum yield were both high (|gCPL| = 1.3 × 10⁻², Φf = 0.17) in the solution phase.
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Kubo et al. (2021) studied this question.
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