Utilizing the polarized light from CPL materials matching the handedness of circularly polarized antiglare filter will improve the energy efficiency and contrast ratio of display devices. Therefore, it is significant to develop OLED materials with excellent chiroptical properties. Currently, two mainstream strategies have been used to design circularly polarized OLEDs (CP-OLEDs) combining CPL and thermally activated delayed fluorescence (TADF) properties. [9,10] The first is the intrinsic chirality strategy, in which the designed chiral element also serves as the luminescent center in the fluorophore. [11][12][13][14] Although relatively high circularly polarized luminescence dissymmetry factor (g PL ) can be obtained by intrinsic chirality of the emitter, it is generally complicated in molecular design, synthesis, and chiral separation with limited molecular structures available. [15,16] The second is the chiral perturbation strategy, that is, the chiral unit does not participate in luminescence, but is placed in close proximity of the fluorophore to induce chiroptical properties. [17][18][19][20] Despite that it is easy to prepare CPL materials with commercially available enantiomers without chiral column separation, their circularly polarized electroluminescence dissymmetry factors (g EL ) are only at the level of 10 −4 -10 −3 , [21,22] which is far from the level of the polymer, [23,24] crystalline complex, [25] and other systems. [26] Therefore, it is highly important and urgent to develop a novel design strategy to improve the g EL in CP-OLEDs.The luminescence dissymmetry factor, g lum , can be given by: [27]