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掺杂有机固体中光电导率起源处的超快电荷转移动力学

Ultrafast Charge Transfer Dynamics at the Origin of Photoconductivity in Doped Organic Solids.

作者信息

Tsokkou Demetra, Cheng Chiao-Yu, Krainova Nina, Mukhopadhyay Sukrit, Giebink Noel C, Banerji Natalie

机构信息

Department of Chemistry and Biochemistry, University of Bern, Freiestrasse 3, 3012 Bern, Switzerland.

Department of Electrical Engineering, The Pennsylvania State University, University Park, Pennsylvania 16802, United States.

出版信息

J Phys Chem C Nanomater Interfaces. 2021 Apr 8;125(13):7086-7096. doi: 10.1021/acs.jpcc.1c01990. Epub 2021 Mar 29.

DOI:10.1021/acs.jpcc.1c01990
PMID:33859770
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC8040020/
Abstract

In spite of their growing importance for optoelectronic devices, the fundamental properties and photophysics of molecularly doped organic solids remain poorly understood. Such doping typically leads to a small fraction of free conductive charges, with most electronic carriers remaining Coulombically bound to the ionized dopant. Recently, we have reported photocurrent for devices containing vacuum-deposited TAPC (1,1-bis(4-bis(4-methylphenyl)aminophenyl)cyclohexane) doped with MoO, showing that photoexcitation of charged TAPC molecules increases the concentration of free holes that contribute to conduction. Here, we elucidate the excited-state dynamics of such doped TAPC films to unravel the key mechanisms responsible for this effect. We demonstrate that excitation of different electronic transitions in charged and neutral TAPC molecules allows bound holes to overcome the Coulombic attraction to their MoO counterions, resulting in an enhanced yield of long-lived free carriers. This is caused by ultrafast back-and-forth shuffling of charges and excitation energy between adjacent cations and neutral molecules, competing with relatively slow nonradiative decay from higher excited states of TAPC. The light-induced generation of conductive carriers requires the coexistence of cationic and neutral TAPC, a favorable energy level alignment, and intermolecular interactions in the solid state.

摘要

尽管分子掺杂有机固体对光电器件的重要性日益增加,但其基本性质和光物理过程仍知之甚少。这种掺杂通常会导致一小部分自由传导电荷,大多数电子载流子仍通过库仑力与电离掺杂剂结合。最近,我们报道了含有真空沉积的掺杂MoO的TAPC(1,1-双(4-双(4-甲基苯基)氨基苯基)环己烷)的器件产生的光电流,表明带电TAPC分子的光激发增加了有助于传导的自由空穴浓度。在这里,我们阐明了这种掺杂TAPC薄膜的激发态动力学,以揭示造成这种效应的关键机制。我们证明,带电和中性TAPC分子中不同电子跃迁的激发使束缚空穴能够克服对其MoO抗衡离子的库仑吸引力,从而提高长寿命自由载流子的产率。这是由相邻阳离子和中性分子之间电荷和激发能的超快来回洗牌引起的,与TAPC较高激发态相对较慢的非辐射衰变相互竞争。光诱导产生导电载流子需要阳离子和中性TAPC共存、有利的能级排列以及固态中的分子间相互作用。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4462/8040020/0c090984ea0d/jp1c01990_0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4462/8040020/41162c00eaa7/jp1c01990_0001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4462/8040020/a8a7bb5daf2b/jp1c01990_0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4462/8040020/6b09dd187f28/jp1c01990_0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4462/8040020/f9d49d65a906/jp1c01990_0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4462/8040020/0c090984ea0d/jp1c01990_0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4462/8040020/41162c00eaa7/jp1c01990_0001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4462/8040020/a8a7bb5daf2b/jp1c01990_0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4462/8040020/6b09dd187f28/jp1c01990_0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4462/8040020/f9d49d65a906/jp1c01990_0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4462/8040020/0c090984ea0d/jp1c01990_0005.jpg

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Polaron Photoconductivity in the Weak and Strong Light-Matter Coupling Regime.弱光与强光物质耦合 regime 下的极化子光电导性 。 (注:这里“regime”可结合上下文灵活翻译,比如“状态”“ regime”等,这里直接保留原文是因为不确定具体最合适的译法,需结合完整文本语境)
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