The biggest challenge is how to improve the efficiency of OLEDs and simultaneously maintain the device stability at high luminance/current density. As for conventional fluorescence materials, only 25% of singlet excitons can be utilized according to spin statistics, which leads to low device efficiency. [2] To harvest other 75% triplet excitons, the new generation of pure organic emitter materials, including thermally activated delayed fluorescence (TADF), [3] triplet-triplet annihilation (TTA), [4] and "hot exciton" materials, [5] have been developed to improve the exciton utilization by converting the triplet excitons to singlet excitons. Nevertheless, during the electroluminescence (EL) process, the accumulation of long-lived triplet excitons usually results in triplet-triplet and/or triplet-singlet quenching, and in turn, the device efficiency suffers serious roll-off, especially at high current density. [6] In addition, these high-activity lowest triplet excited state (T 1 ) excitons adversely influence the surrounding organic materials, leading to material degradation. Thus, the effective way to solve this problem is to accelerate the conversion of triplet to singlet manifold to avoid triplet excitons accumulation.As for conventional TADF materials, a donor-acceptor (D-A)-type molecular design strategy is usually adopted to realize the spatial separation of frontier molecular orbital (FMO), which endows the materials with an extremely small splitting energy between the lowest singlet (S 1 ) and triplet excited states (ΔE ST ). [7] However, the same charge transfer (CT) character of the S 1 ( 1 CT) and T 1 ( 3 CT) states often leads to negligible spin-orbit coupling (SOC) (usually less than 0.1 cm −1 ), which makes the reverse intersystem crossing (RISC) from T 1 to S 1 slow. [8] Thus, the RISC rate constants are usually <10 6 s −1 for most TADF emitters, and the efficiencies of corresponding devices seriously dropped even at low luminance intensity of <1000 cd m −2 . [9] Although great efforts have been made to promote RISC rates, stable TADF-based blue OLEDs are still rarely reported. [10] Different from the TADF materials with the RISC process from T 1 to S 1 , materials with a "hot exciton" mechanism have been proposed that can also theoretically achieve 100% exciton utilization efficiency (EUE) through the RISC process from the high-lying triplet states (T n , n ≥ 2) to the singletstate (S m , m ≥ 1) (hRISC). [11] Compared to the RISC process of The reverse intersystem crossing (RISC) process from triplet to singlet manifold can efficiently improve the efficiencies of organic light-emitting diodes (OLEDs). The relevant RISC rate (k RISC ) is one of the key factors that affect the efficiency roll-off and stability of devices. Here, a new blue "hot exciton" material, CPPCN, with pyrene as the core, is designed and synthesized. Photophysical studies indicate there are multiple high-lying triplet states near the lowest singlet excited state (S 1 ) of CPPCN, which facilitate the RISC from the high-lying...