Hole-transport comparison between solution-processed and vacuum-deposited organic semiconductors

Charge transport in the amorphous organic small molecules α-NPD (N,N′-di(1-naphthyl)-N,N′-diphenyl-(1,1′-biphenyl)-4,4′-diamine) and Spiro-TAD (2,2′,7,7′-tetrakis(N,N-diphenylamino)-9,9-spirobifluorene) is investigated in solution-processed films and compared to charge transport in vacuum-deposited...

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Main Authors: Deepthi K. Mangalore, Paul W. M. Blom, Gert-Jan A. H. Wetzelaer
Format: Article
Language:English
Published: AIP Publishing LLC 2019-01-01
Series:APL Materials
Online Access:http://dx.doi.org/10.1063/1.5058686
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spelling doaj-1f12397c8c6842f8979782419d54b5232020-11-24T21:54:48ZengAIP Publishing LLCAPL Materials2166-532X2019-01-0171011105011105-510.1063/1.5058686002901APMHole-transport comparison between solution-processed and vacuum-deposited organic semiconductorsDeepthi K. Mangalore0Paul W. M. Blom1Gert-Jan A. H. Wetzelaer2Max Planck Institute for Polymer Research, Ackermannweg 10, 55128 Mainz, GermanyMax Planck Institute for Polymer Research, Ackermannweg 10, 55128 Mainz, GermanyMax Planck Institute for Polymer Research, Ackermannweg 10, 55128 Mainz, GermanyCharge transport in the amorphous organic small molecules α-NPD (N,N′-di(1-naphthyl)-N,N′-diphenyl-(1,1′-biphenyl)-4,4′-diamine) and Spiro-TAD (2,2′,7,7′-tetrakis(N,N-diphenylamino)-9,9-spirobifluorene) is investigated in solution-processed films and compared to charge transport in vacuum-deposited films of the same molecule. By optimizing the solution-deposition conditions, such as solvent and concentration, equal charge-transport parameters for solution-processed and vacuum-deposited films are demonstrated. Modeling of the charge carrier transport characteristics was performed by drift-diffusion simulations. The dependence of the charge carrier mobility on temperature, carrier density, and electric field was found to be the same for vacuum deposition and solution processing. In both material processing cases, hole mobilities of 4 × 10−8 m2 V−1 s−1 for spiro-TAD and 0.9 × 10−8 m2 V−1 s−1 for α-NPD are obtained, demonstrating that solution processing can be a viable alternative to vacuum deposition in terms of charge transport.http://dx.doi.org/10.1063/1.5058686
collection DOAJ
language English
format Article
sources DOAJ
author Deepthi K. Mangalore
Paul W. M. Blom
Gert-Jan A. H. Wetzelaer
spellingShingle Deepthi K. Mangalore
Paul W. M. Blom
Gert-Jan A. H. Wetzelaer
Hole-transport comparison between solution-processed and vacuum-deposited organic semiconductors
APL Materials
author_facet Deepthi K. Mangalore
Paul W. M. Blom
Gert-Jan A. H. Wetzelaer
author_sort Deepthi K. Mangalore
title Hole-transport comparison between solution-processed and vacuum-deposited organic semiconductors
title_short Hole-transport comparison between solution-processed and vacuum-deposited organic semiconductors
title_full Hole-transport comparison between solution-processed and vacuum-deposited organic semiconductors
title_fullStr Hole-transport comparison between solution-processed and vacuum-deposited organic semiconductors
title_full_unstemmed Hole-transport comparison between solution-processed and vacuum-deposited organic semiconductors
title_sort hole-transport comparison between solution-processed and vacuum-deposited organic semiconductors
publisher AIP Publishing LLC
series APL Materials
issn 2166-532X
publishDate 2019-01-01
description Charge transport in the amorphous organic small molecules α-NPD (N,N′-di(1-naphthyl)-N,N′-diphenyl-(1,1′-biphenyl)-4,4′-diamine) and Spiro-TAD (2,2′,7,7′-tetrakis(N,N-diphenylamino)-9,9-spirobifluorene) is investigated in solution-processed films and compared to charge transport in vacuum-deposited films of the same molecule. By optimizing the solution-deposition conditions, such as solvent and concentration, equal charge-transport parameters for solution-processed and vacuum-deposited films are demonstrated. Modeling of the charge carrier transport characteristics was performed by drift-diffusion simulations. The dependence of the charge carrier mobility on temperature, carrier density, and electric field was found to be the same for vacuum deposition and solution processing. In both material processing cases, hole mobilities of 4 × 10−8 m2 V−1 s−1 for spiro-TAD and 0.9 × 10−8 m2 V−1 s−1 for α-NPD are obtained, demonstrating that solution processing can be a viable alternative to vacuum deposition in terms of charge transport.
url http://dx.doi.org/10.1063/1.5058686
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