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基于双层发射朗缪尔-布洛杰特膜的有机电致发光二极管。

Dual-emitting Langmuir-Blodgett film-based organic light-emitting diodes.

机构信息

Instituto de Ciencia Molecular, Universidad de Valencia, 46980 Paterna, Spain.

出版信息

Langmuir. 2010 Jul 6;26(13):11461-8. doi: 10.1021/la100956w.

Abstract

Langmuir-Blodgett (LB) films containing alternating layers of the metallosurfactants bis(4,4'-tridecyl-2,2'-bipyridine)-(4,4'-dicarboxy-2,2'-bipyridine) ruthenium(II)-bis(chloride) (1) and bis2-(2,4-difluorophenyl)pyridineiridium(III) chloride (2) have been prepared. Langmuir monolayers at the air-water interface of 1 and 2 with different anions in the subphase have been characterized by pi-A compression isotherms and Brewster angle microscopy (BAM). The transferred LB films have been characterized by IR, UV-vis and emission spectroscopy, and atomic force microscopy (AFM). Electroluminescent devices formed by LB films containing alternating layers of these two molecules show dual emission by simple mixing of the two emitters in a single LB film, and by preparing two stacked configurations, in which a LB layer of the ruthenium complexes is deposited on top of a LB layer of the iridium complexes and the inverse situation. The color of the electroluminescence can be tuned by changing the thickness of each LB layer. Due to efficient hole blocking of a layer of the iridium complexes when deposited on top of the layer of ruthenium complexes, in that configuration the green emission of the iridium complexes is suppressed. In the opposite case, excitons are generated in both layers although most likely preferentially in the layer of the iridium complexes.

摘要

已制备了交替层包含金属表面活性剂双(4,4'-十三烷基-2,2'-联吡啶)-(4,4'-二羧酸-2,2'-联吡啶)钌(II)-双(氯化物)(1)和双[2-(2,4-二氟苯基)吡啶](4,4'-十一烷基-2,2'-联吡啶)铱(III)氯化物(2)的 Langmuir-Blodgett(LB)膜。通过 π-A 压缩等温线和布鲁斯特角显微镜(BAM)对亚相中具有不同阴离子的 1 和 2 的空气 - 水界面的 Langmuir 单层进行了表征。通过 IR、UV-vis 和发射光谱以及原子力显微镜(AFM)对转移的 LB 膜进行了表征。由这些两种分子的交替层形成的电致发光器件通过在单个 LB 膜中简单混合两种发射器来实现双发射,并且通过制备两种堆叠配置来实现,其中 LB 层的钌配合物沉积在 LB 层的铱配合物的顶部,反之亦然。通过改变每个 LB 层的厚度可以调节电致发光的颜色。由于当沉积在 Ru 配合物层的顶部时 Ir 配合物层的空穴阻挡效率很高,因此在该配置中,Ir 配合物的绿色发射被抑制。在相反的情况下,尽管很可能优先在 Ir 配合物层中,但在两个层中都产生激子。

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