Devices based on deep-blue emitting iridium (III) complexes with N-heterocyclic carbene (NHC) ligands have recently been shown to give excellent performance as phosphorescent organic light-emitting diodes (PHOLEDs). To facilitate the design of even better deep-blue phosphorescent emitters we carried out density functional theory (DFT) calculations of the lowest triplet ($T_1$) potential-energy surfaces (PES) upon lengthening the iridium-ligand (Ir-C) bonds. Relativistic time dependent-DFT (TDDFT) calculations demonstrate that this changes the nature of $T_1$ from a highly-emissive metal-to-ligand charge transfer ($^3$MLCT) state to a metal centered ($^3$MC) state where the radiative decay rate is orders of magnitude slower than that of the $^3$MLCT state. We identify the elongation of an Ir-C bond on the NHC group as the pathway with lowest energy barrier between the $^3$MLCT and $^3$MC states for all complexes studied and show that the barrier height is correlated with the experimentally measured non-radiative decay rate. This suggests that the thermal population of $^3$MC states is the dominant non-radiative decay mechanism at room temperature. We show that the $^3$MLCT $\rightarrow$ $^3$MC transition is reversible, in marked contrast to other deep blue phosphors containing coordinating nitrogen atoms, where the population of $^3$MC states breaks Ir-N bonds. This suggests that, as well as improved efficiency, blue PHOLEDs containing phosphors where the metal is only coordinated by carbon atoms will have improved device lifetimes.
Comment: 15 pages, 4 figures, 3 tables