Triplet-exciton quenching in organic phosphorescent light-emitting diodes with Ir-based emitters
Triplet-exciton quenching in organic phosphorescent light-emitting diodes with Ir-based emitters
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DOI:
10.1103/physrevb.75.125328
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发表时间:
2007-03-01
影响因子:
3.7
通讯作者:
Leo, Karl
中科院分区:
文献类型:
--
作者:
Reineke, Sebastian;Walzer, Karsten;Leo, Karl
We investigate quenching processes which contribute to the roll-off in quantum efficiency of phosphorescent organic light-emitting diodes (OLED's) at high brightness: triplet-triplet annihilation, energy transfer to charged molecules (polarons), and dissociation of excitons into free charge carriers. The investigated OLED's comprise a host-guest system as emission layer within a state-of-the-art OLED structure-i.e., a five-layer device including doped transport and thin charge carrier and exciton blocking layers. In a red phosphorescent device, N,N-'-di(naphthalen-2-yl)- N,N-'-diphenyl-benzidine is used as matrix and tris(1-phenylisoquinoline) iridium [Ir(piq)(3)] as emitter molecule. This structure is compared to a green phosphorescent OLED with a host-guest system comprising the matrix 4,4('),4(')-tris (N-carbazolyl)-triphenylamine and the well-known triplet emitter fac-tris(2-phenylpyridine) iridium [Ir(ppy)(3)]. The triplet-triplet annihilation is characterized by the rate constant k(TT) which is determined by time-resolved photoluminescence experiments. To investigate triplet-polaron quenching, unipolar devices were prepared. A certain exciton density, created by continuous-wave illumination, is analyzed as a function of current density flowing through the device. This delivers the corresponding rate constant k(P). Field-induced quenching is not observed under typical OLED operation conditions. The experimental data are implemented in an analytical model taking in account both triplet-triplet annihilation and triplet-polaron quenching. It shows that both processes strongly influence the OLED performance. Compared to the red Ir(piq)(3) OLED, the green Ir(ppy)(3) device shows a stronger efficiency roll-off which is mainly due to a longer phosphorescent lifetime tau and a thinner exciton formation zone w.