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具有石墨烯阴极的高效小分子有机发光二极管,该阴极覆盖有具有纳米凹坑的 Sm 层,并在凹坑中通过 Bphen:CsCO 进行 n 型掺杂。

Efficient small molecular organic light emitting diode with graphene cathode covered by a Sm layer with nano-hollows and n-doped by Bphen:CsCO in the hollows.

机构信息

State Key Laboratory for Microscopic Physics, School of Physics, Peking University, Beijing 100871, People's Republic of China.

出版信息

Nanotechnology. 2017 Mar 10;28(10):105201. doi: 10.1088/1361-6528/aa55e5. Epub 2016 Dec 28.

DOI:10.1088/1361-6528/aa55e5
PMID:28028246
Abstract

Graphene is a favorable candidate for electrodes of organic light emitting diodes (OLEDs). Graphene has quite a high work function of ∼4.5 eV, and has been extensively studied when used as anodes of OLEDs. In order to use graphene as a cathode, the electron injection barrier between the graphene cathode and the electron transport layer has to be low enough. Using 4,7-diphenyl-1,10-phenanthroline (Bphen):CsCO to n-dope graphene is a very good method, but the electron injection barrier between the n-doped graphene and Bphen:CsCO is still too high to be ∼1.0 eV. In this work, in order to further reduce the electron injection barrier, a novel method is suggested. On the graphene cathode, a Sm layer with a lot of nano-hollows, and subsequently a layer of Bphen:CsCO, are deposited. The Bphen:CsCO can n-dope graphene in the nano-hollows, and the Fermi level of the graphene rises. The nano Sm layer is very easily oxidized. Oxygen adsorbed on the surface of graphene may react with Sm to form an O-Sm dipole layer. On the areas of the Sm oxide dipole layer without nano-hollows, the electron injection barrier can be further lowered by the dipole layer. Electrons tend to mainly inject through the lower electron barrier where the dipole layer exists. Based on this idea, an effective inverted small molecular OLED with the structure of graphene/1 nm Sm layer with a lot of nano-hollows/Bphen:CsCO/Alq:C545T/NPB/MoO/Al is presented. The maximum current efficiency and maximum power efficiency of the OLED with a 1 nm Sm layer are about two and three times of those of the reference OLED without any Sm layer, respectively.

摘要

石墨烯是有机发光二极管(OLED)电极的理想候选材料。石墨烯的功函数相当高,约为 4.5eV,当用作 OLED 的阳极时,已经得到了广泛的研究。为了将石墨烯用作阴极,石墨烯阴极与电子传输层之间的电子注入势垒必须足够低。使用 4,7-二苯基-1,10-菲咯啉(Bphen):CsCO 对石墨烯进行 n 掺杂是一种非常好的方法,但 n 掺杂石墨烯与 Bphen:CsCO 之间的电子注入势垒仍然过高,约为 1.0eV。在这项工作中,为了进一步降低电子注入势垒,提出了一种新方法。在石墨烯阴极上沉积了一层具有大量纳米凹坑的 Sm 层,随后沉积了一层 Bphen:CsCO。Bphen:CsCO 可以在纳米凹坑中对石墨烯进行 n 掺杂,使石墨烯的费米能级升高。纳米 Sm 层很容易被氧化。吸附在石墨烯表面的氧可能与 Sm 反应形成 O-Sm 偶极子层。在没有纳米凹坑的 Sm 氧化物偶极子层的区域,偶极子层可以进一步降低电子注入势垒。电子倾向于主要通过存在偶极子层的较低电子势垒注入。基于这一思路,提出了一种有效的倒置小分子 OLED,其结构为石墨烯/1nm Sm 层具有大量纳米凹坑/Bphen:CsCO/Alq:C545T/NPB/MoO/Al。具有 1nm Sm 层的 OLED 的最大电流效率和最大功率效率分别约为没有任何 Sm 层的参考 OLED 的两倍和三倍。

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