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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Online Access: | http://dx.doi.org/10.1063/1.5058686 |
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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 |
work_keys_str_mv |
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