Intense research is currently directed towards polymer light-emitting diodes (PLEDs) because of their potential for application in flat-panel displays. [1,2] Based on their compatibility with solution processing, the exploration of their suitability for organic electronic devices has primarily been motivated by the need for low-cost production over large areas by utilizing spin-coating, ink-jet printing, or screenprinting technologies. According to simple statistics, the process of charge injection and recombination in PLEDs generates singlet excitons with a quantum efficiency of only 25 %, setting an upper limit to the efficiency of PLEDs based on fluorescent polymers. Even though the singlet±triplet ratio in PLEDs is still a topic of debate, [3±6] it is expected that the radiative decay of both singlet and triplet states would substantially increase the efficiency of PLEDs. Phosphorescent dyes have been used to overcome the efficiency limit imposed by the unavoidable formation of triplet excitons, and highly efficient phosphorescent light-emitting diodes based on low molecular weight materials have been demonstrated.[7±9]These high-efficiency devices typically consist of several layers including a hole-transporting layer, an emission layer doped with the phosphorescent dye, an exciton-/hole-blocking layer and an electron-injecting layer. In fact, a multilayer LED utilizing fac-tris(2-phenylpyridine)iridium (Ir(ppy) 3 ) as the emitting species exhibited a very high external quantum efficiency (EQE) of 19.2 % and a power conversion efficiency (PCE) of 72 lm W ±1 at 65 cd m ±2 .[9]Polymer phosphorescent light-emitting diodes (PPLEDs) usually utilize a phosphorescent dye doped into a chargetransporting polymer matrix.[10±17] One of the criteria for the selection of the polymer matrix is that the energy of the lowest lying triplet state (T 1 ) of the host is larger or at least comparable to that of the phosphorescent guest. In case of Ir(ppy) 3 with a triplet energy of about 2.4 eV, mostly non-conjugated polymers, such as poly(N-vinyl-carbazole) (PVK), have been used. [11±16] In order to optimize the balance of charge-carrier injection and transport and to confine the emissive triplet excitons within the emission layer, the structure of PPLEDs generally resembles that of low molecular weight material multilayer devices.[11±15] Yang and Tsutsui were the first to publish an efficient multilayer PPLED with a PVK:Ir(ppy) 3 emission layer and an evaporated low molecular weight electron-transporting layer.[11] These devices exhibited an external quantum efficiency of up to 7.5 %. A luminance of 100 cd m ±2 was reached at about 14 V and the power conversion efficiency was 5.8 lm W ±1 under these conditions.Lamansky et al. [14] achieved EQEs of 3.4 % in single-layer structures by adding the low molecular weight electron-transporting molecule 2-(4-biphenylyl)-5-(4-tert-butylphenyl)-1,3,4-oxadiazole (PBD) to the PVK host to facilitate electron transport. Vaeth and Tang [15] reported an EQE of 8.5 % and a PCE of 9.9 lm W ±1 ...