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Study on Charge Carrier Recombination Zone with Ultrathin Rubrene Layer as Probe

机译:以超薄钌层为探针的载流子复合区研究

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The characteristic of charge carrier recombination zone in N,N'-bis-(1-naphthyl)-N,N'-biphenyl-1,1'-biphenyl-4,4'-diamine (NPB) based OLEDs is studied using an ultrathin 5,6,11,12-tetraphenylnaphthacene (rubrene) as a probe. By adjusting the rubrene thickness and location in NPB light-emitting layer, the luminescent spectra and electrical properties of the devices are investigated. The results show that when the thickness ranges from 0.2 to 0.8 nm, the surface morphology of rubrene exists as the discontinuous island-like state locating on the surface of NPB film and seldom affect the electrical characteristics. While the location of rubrene shifted from the interface of NPB/2,9-dimethyl-4,7-diphenyl-1,10-phenanthroline (BCP) to NPB side, the maximum exciton concentration is found within 2 nm away from the interface, which is the main charge carrier recombination zone. With an optimized structure of indium-tin-oxide (ITO)/NPB (40nm)/rubrene (0.3nm)/NPB (7nm)/BCP (30nm)/Mg:Ag, the device exhibits a turn on voltage as low as 3 V and stable white light. The peaks of EL spectra are located at 431 and 555 nm corresponding to the Commissions Internationale De L'Eclairage (CIE) coordinates of (0.32, 0.32), which are relatively stable under the bias voltage from 5 to 15 V. A maximum luminance of 5630 cd/m~2 and a maximum power efficiency of 0.6 lm/W is achieved. The balanced spectra are attributed to the stable confining of charge carriers and exciton by the thin emitting layers.
机译:N,N'-双-(1-萘基)-N,N'-联苯-1,1'-联苯-4,4'-二胺(NPB)基OLED中的电荷载流子复合区特性研究使用超薄的5,6,11,12-四苯基萘(rubrene)作为探针。通过调节红荧烯的厚度和在NPB发光层中的位置,研究了器件的发光光谱和电性能。结果表明,当厚度为0.2〜0.8nm时,红荧烯的表面形态以NPB膜表面不连续的岛状存在,几乎不影响电学性能。虽然红荧烯的位置从NPB / 2,9-二甲基-4,7-二苯基-1,10-菲咯啉(BCP)的界面转移到NPB一侧,但在距界面2 nm处发现了最大激子浓度,这是主要的电荷载流子复合区。利用氧化铟锡(ITO)/ NPB(40nm)/钌(0.3nm)/ NPB(7nm)/ BCP(30nm)/ Mg:Ag的优化结构,该器件的开启电压低至3 V和稳定的白光。 EL光谱的峰值位于431和555 nm处,对应于(0.32,0.32)的国际照明委员会(CIE)坐标,在5至15 V的偏置电压下相对稳定。达到5630 cd / m〜2,最大功率效率为0.6 lm / W。平衡的光谱归因于薄发射层对载流子和激子的稳定限制。

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