success of these applications. Fluorescent OLEDs can only convert 25% of singlet excitons into emission, with the loss of 75% triplet excitons as heat. [2] In the past decade, thermally activated delayed fluorescence (TADF) materials have emerged as emitters for the third-generation OLED, able to harvest 100% of excitons to generate light, at comparable exciton utilization efficiencies to phosphorescent OLEDs. Generally, TADF emitters are based on a strongly twisted donor-acceptor (D-A) design motif to electronically separate the highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO) that results in a small energy gap between S 1 and T 1 states (ΔE S1T1 ). [3][4][5] However, a relatively large nuclear reorganization and charge-transfer (CT) transition in the excited state unavoidably produces a broad emission band, reflected by a large full width at half maximum (FWHM) of around 100 nm. [6] These undesired properties in D-A TADF emitters restrict their practical application in high-resolution displays where the color point requirements demanded by industry are difficult to obtain using materials showing broad emission.At present, commercialized high-resolution OLED displays mainly employ a color filter or microcavity to reach the color purity required by broadcasting standards, which is inevitably accompanied by losses in device efficiency and energy utilization. [7] Therefore, it would be of great utility to devise an emitter showing narrowband emission. Recently, Hatakeyama et al. introduced a subclass of TADF emitters coined multi-resonant TADF (MR-TADF), that shows the desired narrowband emission. This is due to their rigid polyaromatic hydrocarbon (PAH) framework, [8] where the rigid molecular skeleton and the shortrange CT (SRCT) nature of the emissive singlet excited state enable simultaneously narrowband emission and small ΔE S1T1 . In this design, the electron densities of the HOMO and LUMO are localized on the adjacent atoms. Typically, boron/nitrogen (B/N) doped PAHs have emerged as the dominant design. For example, Hatakeyama and co-workers designed a B/N-doped MR-TADF compound, ν-DABNA, that shows very narrowband emission (FWHM of 18 nm) at a photoluminescence (PL) maximum (λ PL ) of 467 nm, with a PL quantum yield (Φ PL ) of 90%, and where the device's maximum external quantum efficiency The S 1 state and high-lying triplet excited states (ΔE S1Tn ) offer insight into clarifying the mechanism of efficiency roll-off of organic light-emitting diodes (OLEDs). However, experimental detection of the ΔE S1Tn is challenging due to Kasha's rule. Here, two emitters, PhCz-O-DiKTa and PhCz-DiKTa, showing multi-resonant thermally activated delayed fluorescence (MR-TADF) are reported. By modulating the conjugation between the MR-TADF DiKTa emissive center and donor substituent, emission directly from the T 2 state is for the first time observed in MR-TADF emitters. Single crystal and reduced density gradient analyses reveal the origin of the reduced observed concentrationquenchi...