“…For the LE state, the distribution positions of electrons and holes before and after electron transition are roughly the same, and this excited state often appears in conjugated rigid molecules, such as pyrenes and anthracenes. ,, In contrast, for the CT state, the electrons and holes are distributed on the different fragments of the molecule before and after electron transition, which often appears in the donor–acceptor (D–A) or D−π–A compounds. − The molecules dominated by the LE state generally have high radiation transition rates and photoluminescence efficiency, but the larger exciton binding energy affects the spin flip of electrons, resulting in a lower exciton utilization rate. Although the molecules dominated by the CT state can effectively improve exciton utilization, they are usually accompanied by weak luminous intensity. − Therefore, designing molecules with both LE and CT states can not only ensure the radiation efficiency of the energy but also increase the utilization rate of excitons. , Based on the above considerations, herein, four new D–A pyranone–arylbenzene molecules were designed and synthesized (Scheme ), in which pyranone ( Pr ) was selected as the acceptor to ensure that the molecules had the CT state, whereas benzene ( Ph ), naphthalene ( Np ), anthracene ( An ), and pyrene ( Py ) were used as donors to increase the LE state. Solvatochromic experiments, single-crystal structures, theoretical calculations, and low-temperature delayed emissions demonstrate that Pr – Ph and Pr – Np mainly have the twisted intramolecular charge-transfer (TICT) state in the excited state, and thus, these two compounds show very weak fluorescence emissions in solution.…”