basically limited to donor (D)-π-acceptor (A) molecular architecture. [2] This type of molecular design, first proposed by Adachi and co-workers for TADF, [1a] can tune their D or/and A groups, geometries, and steric hindrance between them to generate twisted induced charge-transfer-type emission. [3] The twisted dihedral angle between D and A units can minimize the singlettriplet splitting energy (ΔE ST) for fast RISC, [1c,4] but the resulted TADF OLEDs still need to be significantly improved, notably in terms of efficiency roll-off at high brightness and concentration quenching because of the ππ intermolecular interactions in the solid-state. [5] Another way to achieve TADF is to use D/A complex, in which the D/A blocks are spatially isolated, but their forming exciplexes are far less efficient than D-π-A analogs, and the resulting OLEDs also display severe efficiency roll-off. [6] Recently, researchers conceptually consider that the intramolecular noncovalent interaction between D/A units in faceto-face alignment could be a new option to realize TADF. [7] Constructing TADF materials in this unconjugated way has the potential to combine the small ΔE ST value with substantial transition dipole and achieve high luminescent efficiency. [8] These two electron-rich and electron-poor π-systems need to be held close in space to form homoconjugation. In this regard, The ORCID identification number(s) for the author(s) of this article can be found under