In this contribution a detailed mechanistic investigation of merto-fac photoisomerization occurring in Ir(ppy) 3 (ppy = 2-phenylpyridine) is presented. Facial/meridional stereoisomerism in trisbidentate Ir(III) complexes strongly determines their photophysical properties and thereby their efficiency and stability within a phosphorescence-based organic light-emitting diode (PhOLED) device. Double-hybrid density functional theory (DFT) calculations are performed herein to identify the photoactive species involved in the photoisomerization reaction and to assess its kinetic and thermodynamic feasibility at room temperature. These investigations highlight the protagonistic role of a non-previously described 3 MC (triplet metal-centred) state bearing one stretched trans Ir-N position. Finally, and in view of the computed evidences, phosphor design strategies to prevent photoisomerization are proposed.Organometallic complexes of Ir(III) and/or Pt(II) are widely used as efficient phosphors for phosphorescent-based organic lightemitting diodes (PhOLEDs). [1,2] To further improve their device operational lifetimes, and especially in the case of blue phosphors, it is crucial to acquire durable and efficient materials that do not suffer intrinsic chemical degradation upon PhOLED operation. [3][4][5][6][7][8] Degradation of PhOLEDs' materials originates from parasitic exciton-polaron and exciton-exciton annihilation processes, [4,7] such as e. g., triplet-triplet annihilation (TTA) and triplet-polaron annihilation (TPA), which also compromise PhOLEDs efficiency at high brightness levels (i. e., roll-off effect). [9] In recent years, numerous computational [10][11][12] and experimental [13][14][15][16] efforts have been made to decipher the underlying degradation mechanisms, and still many open questions remain. In the case of phosphors, ligand dissociation reactions are the most common degradation routes. [7,16] These reactions lead to the formation of products in an irreversible manner that act as nonradiative recombination sites, charge traps and/or luminescence quenchers. Thus, these final products are ultimately responsible for the significant luminance loss in the aged devices. Evidence shows that the population of higher-lying excited states, and particularly, triplet metalcentered ( 3 MC) excited states, [10,16] strongly enhances these degradation processes. 3 MC states are usually highly distorted with respect to the ground state ( 1 GS) and lowest triplet (T 1 ) excited state geometries, [17] the latter typically being of predominant metal-to-ligand charge transfer character, i. e., 3 MLCT. For instance, in cyclometalated Ir(III) complexes, both 1 GS and T 1 exhibit a pseudo-octahedral geometrical disposition while the 3 MC state often displays a pentacoordinate trigonal bipyramid arrangement bearing one broken IrÀ N bond. [17,18] Therefore, ligand dissociation is more likely to occur from a 3 MC state than from either 1 GS or T 1 . As recently disclosed, the excited state potential energy surfaces (PES) of these co...