After the first report of organometallic complex-based phosphorescent emitting materials, [5] it was possible to realize 100% internal quantum efficiency in phosphorescent OLEDs (PhOLEDs). [6] Using strong spin-orbit coupling (SOC) of heavy metals such as platinum or iridium, it was possible to surpass the limit of spin statistics and utilize all triplet excitons as well as singlet excitons in PhOLEDs. [7-10] After a huge improvement in the external quantum efficiencies (EQEs) in PhOLEDs, it was possible to commercialize green and red PhOLEDs as replacements for green and red fluorescent OLEDs. However, blue fluorescent OLEDs could not be replaced with PhOLEDs due to lifetime issues. [11,12] Although the currently commercialized OLEDs are mainly based on PhOLEDs, serious issues such as high cost, need for rare materials, and environmental sustainability of the phosphorescent emitters used have forced researchers to identify an alternative to PhOLEDs. [13,14] Recently, TADF OLEDs have emerged as a viable alternative to PhOLEDs due to their capability to exhibit 100% internal quantum efficiency (like PhOLEDs) by harvesting both singlet and triplet excitons through a reverse intersystem crossing (RISC) mechanism. [15-19] As the emitters used in TADF OLEDs are purely organic materials, they are inexpensive, readily available, and offer a large number of design opportunities. They can be easily tuned for different colors and can also serve as efficient host materials in the emitting layers. After the first report of a high EQE TADF OLED in 2012, [20] a number of highly efficient blue, green, and red TADF OLEDs have been reported. [21-36] Although short device lifetime and poor color purity are the main obstacles in commercial application of TADF OLEDs, they are promising because they have obtained high EQEs equal to or higher than that of the PhOLEDs. Commercially applicable, highly efficient, stable, and pure color TADF emitters must have four important characteristics of small singlet-triplet energy gap (ΔE ST), high photoluminescence quantum yield (PLQY), small full width at half-maximum (FWHM), and stability of the emitting materials. However, it is difficult to achieve all four factors in a single molecular design. [17] For example, a small ΔE ST can be obtained through separation of the highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO) using highly twisted molecular structures. However, a high PLQY will be realized by maximizing the overlap between the HOMO and LUMO. The two factors are contradictory, but they are necessary Recent developments in purely organic-material-based thermally activated delayed fluorescence (TADF) emitters are helping to make them suitable for commercial applications in the near future. In spite of their high external quantum efficiencies, the broad emission spectra and short device lifetimes are the main barriers to using TADF emitters. Among the classes of materials, boron-embedded polycyclic aromatic compounds have shown potential as TADF emitte...