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High-efficiency red phosphorescent organic light-emitting diodes based on metal-microcavity structure

机译:基于金属微腔结构的高效红色磷光有机发光二极管

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Multilayer electroluminescent (EL) diodes with red emission were fabricated using Bis(2-(2'-benzo[4,5-α]thienyl)pyridinato-N,C~(3')) iridium (acetyl-acetonate) [(btp)_2Ir(acac)] as dopant. Double metal-microcavity structure with a semitransparent Ag anode was introduced into the EL diodes. The cavity device structure was ITO/Ag/N,N'-di(naphthalene-1-yl)-N,N'-diphenyI-benzidine [NPB]/4,4'-N,N'-dicarbazole-biphenyl [CBP]: 5 wt% (btp)_2Ir(acac)/2,2',2"-(1,3,5-benzenetriyl)tris[1-phenyl-1H-benzimidazole] [TPBi]/LiF/Al. The sharp bright red emission of cavity device was observed. Compared with noncavity device the full width at half maximum (FWHM) of top normal emission spectrum was narrowed from 38 nm to 23 nm, and the maximum brightness of the cavity device was increased from 3500 cd/m~2 to 5800 cd/m~2, i.e., was improved by a factor of 1.7. The blue-shift of emission spectrum with increasing detection angle in traditional microcavity device was no longer observed, which attributed to a very steep rising of the EL-emission from (btp)_2Ir(acac). Besides, it was importantly found that at higher current density EL efficiency was obviously higher for the cavity device than for non-cavity device, i.e., at J = 200 mA/cm~2 the former and later were 1.8 cd/A and 1.0 cd/A, respectively. And the increasing mechanism of the EL efficiency was ascribed to the shortened lifetime of triplet excited state (T_1) and the weakened hole injection of Ag anode.
机译:使用双(2-(2'-苯并[4,5-α]噻吩基)吡啶基-N,C〜(3'))铱(乙酰丙酮)[(btp)制备具有红色发射的多层电致发光(EL)二极管)_2Ir(acac)]作为掺杂剂。将具有半透明Ag阳极的双金属微腔结构引入EL二极管。空腔装置的结构为ITO / Ag / N,N'-二(萘-1-基)-N,N'-二苯基-联苯胺[NPB] / 4,4'-N,N'-二咔唑-联苯[CBP ]:5重量%(btp)_2Ir(acac)/ 2,2',2“-(1,3,5-苯三基)三[1-苯基-1H-苯并咪唑] [TPBi] / LiF / Al。观察到腔体器件发出红色亮光,与非腔体器件相比,顶部法向发射光谱的半峰全宽(FWHM)从38 nm缩小至23 nm,腔体器件的最大亮度从3500 cd / m〜2达到5800 cd / m〜2,即提高了1.7倍;不再观察到传统微腔装置中发射光谱随检测角度的增加而出现蓝移,这是由于电子束的陡峭上升所致。 (btp)_2Ir(acac)的EL发射此外,重要的是,发现在较高电流密度下,空腔器件的EL效率明显高于非空腔器件,即在J = 200 mA / cm〜2时前者和后者分别为1.8 cd / A和1.0 cd / A,分别是伊利EL效率的提高机制归因于三重激发态(T_1)寿命的缩短和Ag阳极空穴注入的减弱。

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