The pioneering investigations by Thompson and Forrest introduced fac-tris(2-phenyl pyridine)iridium (Ir(ppy) 3 ) as a highly efficient phosphorescent material because the green emission of Ir(ppy) 3 takes advantage of both electrically generated singlet and triplet excitons.1,2 The luminescence efficiency can be increased to a quantum yield of up tõ 100%, 1-6 which suggests emission-related applications. In general, emission from triplet to singlet states is forbidden but the electrons of Ir(III) can induce a quantum mechanical effect, such as spin-orbit coupling, and allow a phosphorescent transition.1-6 In this regard, most studies have focused on monomeric Ir(ppy) 3 in dilute solution (1 × 10 −5 M) or thin films with a low doping ratio (< 1 wt%), whereas there is little information on the intermolecular interactions of Ir(ppy) 3 molecules.2,3 This Note reports the luminescent properties of neat Ir(ppy) 3 films investigated by temperatureand time-dependent spectroscopy. Three triplet substates were found to be responsible for the phosphorescence. Moreover, energy transfer between Ir(ppy) 3 molecules was observed due to the physical proximity in neat films.The photoluminescence (PL) spectrum of a typical neat Ir(ppy) 3 film at 300 K is shown in Figure 1(a). The emission peak was observed at 509 nm, which is similar to the phosphorescence of Ir(ppy) 3 in solution, [4][5][6] suggesting that the triplet states are the emitting states, even in the neat film. The quantum yield is related to the strength of spin-orbit coupling because the phosphorescence is allowed due to the influence of spin-orbit coupling induced by the heavy center ion, Ir(III). In other words, the triplet state with a large extent of metal-to-ligand charge-transfer (MLCT) state, which involves the 5d orbitals of Ir(III) (the highest occupied molecular orbitals, HOMOs) and the π* orbitals of 2-phenylpyridine (the lowest unoccupied molecular orbitals, LUMOs), 4 would show efficient phosphorescence. The contribution of the MLCT character can be estimated by several ways. One of them is the magnitude of zero-field splitting because it is determined by the strength of spinorbit coupling. The triplet states of Ir(ppy) 3 have a zero-field splitting value of 170 cm −1 in the CH 2 Cl 2 solution, 4 suggesting a large MLCT character. The rigidochromism of the emitting states is another explanation. A blue-shift of emission was observed for a transition of the MLCT state in a rigid condition 5,7 because a charge-transfer transition state was less relaxed by dipolar interactions of the solvents in the rigid condition. An emission peak in the neat film was observed at 509 nm, which was blue-shifted by ~10 nm compared to that in the CH 2 Cl 2 solution, 4 indicating the MLCT character in the emitting triplet states of the neat Ir(ppy) 3 film. The MLCT character was also distinguished by a broad and unstructured spectral shape of the phosphorescence spectrum, 7-9 whereas the ligand-centered (LC) transitions exhibited vibronic fine structures.7-10 The PL spectrum...