2014
DOI: 10.1002/adma.201401476
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High‐Efficiency Fluorescent Organic Light‐Emitting Devices Using Sensitizing Hosts with a Small Singlet–Triplet Exchange Energy

Abstract: Materials with small singlet-triplet splits (ΔEST s) are introduced as sensitizing hosts to excite fluorescent dopants, breaking the trade-off between small ΔEST and high radiative decay rates. A highly efficient orange-fluorescent organic light-emitting diode (OLED) is prepared, showing a maximum external quantum efficiency of 12.2%.

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Cited by 514 publications
(364 citation statements)
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“…The device with 20% 2CzPN produces a maximum forward viewing power efficiency of 50.2 lm W 21 (Figure 3d). Because illumination sources are typically characterized by their total emitted power, our WOLED exhibits a total EQE max of 33.3% and a total PE max of 85.3 lm W 21 (measured using an integrating sphere), which roll off to 22.7% and 34.0 lm W 21 at a high brightness of 1000 cd m 22 . To the best of our knowledge, these values are among the best results reported thus far for hybrid white devices (see Table 1) and are even comparable to the values of all phosphor white devices.…”
Section: Resultsmentioning
confidence: 99%
“…The device with 20% 2CzPN produces a maximum forward viewing power efficiency of 50.2 lm W 21 (Figure 3d). Because illumination sources are typically characterized by their total emitted power, our WOLED exhibits a total EQE max of 33.3% and a total PE max of 85.3 lm W 21 (measured using an integrating sphere), which roll off to 22.7% and 34.0 lm W 21 at a high brightness of 1000 cd m 22 . To the best of our knowledge, these values are among the best results reported thus far for hybrid white devices (see Table 1) and are even comparable to the values of all phosphor white devices.…”
Section: Resultsmentioning
confidence: 99%
“…Generally, efficient reverse intersystem crossing (RISC) process and high fluorescence quantum yield ( Φ F ) are two essential requirements for efficient TADF emitters 1, 5. For the former one, an extremely small singlet‐triplet energy split (Δ E ST ) between lowest singlet excited state (S 1 ) and lowest triplet excited state (T 1 ) is highly desired to up‐convert triplet excitons to singlet excitons through thermal excitation 4, 6, 7, 8, 9, 10.…”
mentioning
confidence: 99%
“…On one hand, PHOLEDs are much more expensive than *Corresponding author (email: duanl@mail.tsinghua.edu.cn) fluorescent OLEDs due to the high cost of phosphors containing rare metals, such as iridium [17,18] and platinum [19] and the high dopant concentration of phosphors (5 wt%-20 wt%) required to achieve optimum device performance [20][21][22][23]; on the other hand, the efficiencies of PHOLEDs tend to decrease with the brightness increasing, which is called efficiency roll-off [24]. Efforts have been paid to solve these problems, such as replacing the high-cost phosphorescent emitters to pure organic ones [25][26][27][28][29][30][31][32], or decreasing the excitons' lifetime and broadening the recombination zone to reduce molecular aggregation [24,[33][34][35], however, the performance of these devices are not satisfactory enough.…”
Section: Introductionmentioning
confidence: 97%