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N, N'-二苯基-N, N'-双(1-萘基)-1, 1'-联苯-4, 4''-二胺薄膜中三重态迁移的动力学。

Dynamics of triplet migration in films of N, N'-diphenyl-N, N'-bis(1-naphthyl)-1, 1'-biphenyl-4, 4''-diamine.

机构信息

OEM Research Group, Department of Physics, University of Durham, Durham DH1 3LE, UK.

出版信息

J Phys Condens Matter. 2010 May 12;22(18):185802. doi: 10.1088/0953-8984/22/18/185802. Epub 2010 Apr 20.

Abstract

We study triplet migration properties in NPB (N, N'-diphenyl-N, N'-bis(1-naphthyl)-1, 1'-biphenyl-4, 4''-diamine) films using time resolved gated spectroscopy and dispersive migration theory as our main tools of analysis. We show that in NPB, a well-known hole transporter in organic light emitting diodes, at high excitation densities triplet migration follows two regimes--a dispersive non-equilibrium regime (distinguished by exciton energetical relaxation within the distribution of hopping sites and as a consequence the hopping frequency being time dependent) that evolves into a second, non-dispersive equilibrium regime. Further, we observe a third region, which we term acceleration. From the turning over time between dispersive and non-dispersive dynamics, we deduce the width of the triplet density of states (DOS). We observe how the DOS variance changes when one decreases the thickness of the NPB film and note how surface effects are becoming important. Furthermore, the DOS variance of NPB changes when another organic layer is evaporated on top, namely Ir(piq)3 (tris(1-phenylisoquinoline)iridium(III)). We believe that these changes are due to the different polarizable media in contact with the NPB film, either vacuum or Ir(piq)3. We also show in this paper that the triplet level when time approaches zero is much higher in energy than the relaxed triplet levels, as quoted in most published papers; these values are thus incorrect for NPB. Lastly, it is possible that even at room temperature, the dispersive regime might be important for triplet migration at high initial triplet concentrations and might affect the diffusion length of triplets to a certain extent. However, more experimentation needs to be performed in order to address this question. Overall, we have characterized the triplet migration dynamics of NPB fully and shown that it agrees with previously published observations for other organic semiconductors and theoretical considerations.

摘要

我们使用时间分辨门控光谱和弥散迁移理论作为主要分析工具,研究了 NPB(N,N'-二苯基-N,N'-双(1-萘基)-1,1'-联苯-4,4''-二胺)薄膜中的三重态迁移特性。我们表明,在 NPB 中,一种众所周知的有机发光二极管空穴传输体,在高激发密度下,三重态迁移遵循两个区域——一个弥散的非平衡区域(通过激子在跳跃位点分布内的能量弛豫来区分,因此跳跃频率随时间变化),然后演变成第二个非弥散的平衡区域。此外,我们观察到第三个区域,我们称之为加速区。从弥散和非弥散动力学之间的翻转时间,我们推断出三重态密度状态(DOS)的宽度。我们观察了当我们减小 NPB 薄膜的厚度时 DOS 方差如何变化,并注意到表面效应变得越来越重要。此外,当在顶部蒸发另一个有机层时,即 Ir(piq)3(三(1-苯基异喹啉)铱(III)),NPB 的 DOS 方差会发生变化。我们认为这些变化是由于与 NPB 薄膜接触的不同极化介质,要么是真空,要么是 Ir(piq)3。我们还在本文中表明,当时间趋近于零时,三重态能级比大多数已发表论文中引用的弛豫三重态能级高得多;因此,这些值对于 NPB 是不正确的。最后,即使在室温下,对于初始三重态浓度较高的三重态迁移,弥散态可能也很重要,并在一定程度上影响三重态的扩散长度。然而,需要进行更多的实验来解决这个问题。总的来说,我们已经充分描述了 NPB 的三重态迁移动力学,并表明它与其他有机半导体的先前发表的观察结果和理论考虑一致。

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