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Downscaling the Sample Thickness to Sub-Micrometers by Employing Organic Photovoltaic Materials as a Charge-Generation Layer in the Time-of-Flight Measurement
Time-of-flight (TOF) measurements typically require a sample thickness of several micrometers for determining the carrier mobility, thus rendering the applicability inefficient and unreliable because the sample thicknesses are orders of magnitude higher than those in real optoelectronic devices. Her...
Autores principales: | , , , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group
2015
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4441200/ https://www.ncbi.nlm.nih.gov/pubmed/25999238 http://dx.doi.org/10.1038/srep10384 |
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author | Liu, Shun-Wei Lee, Chih-Chien Su, Wei-Cheng Yuan, Chih-Hsien Lin, Chun-Feng Chen, Kuan-Ting Shu, Yi-Sheng Li, Ya-Ze Su, Tsung-Hao Huang, Bo-Yao Chang, Wen-Chang Liu, Yu-Hsuan |
author_facet | Liu, Shun-Wei Lee, Chih-Chien Su, Wei-Cheng Yuan, Chih-Hsien Lin, Chun-Feng Chen, Kuan-Ting Shu, Yi-Sheng Li, Ya-Ze Su, Tsung-Hao Huang, Bo-Yao Chang, Wen-Chang Liu, Yu-Hsuan |
author_sort | Liu, Shun-Wei |
collection | PubMed |
description | Time-of-flight (TOF) measurements typically require a sample thickness of several micrometers for determining the carrier mobility, thus rendering the applicability inefficient and unreliable because the sample thicknesses are orders of magnitude higher than those in real optoelectronic devices. Here, we use subphthalocyanine (SubPc):C(70) as a charge-generation layer (CGL) in the TOF measurement and a commonly hole-transporting layer, N,N’-diphenyl-N,N’-bis(1,1’-biphenyl)-4,4’-diamine (NPB), as a standard material under test. When the NPB thickness is reduced from 2 to 0.3 μm and with a thin 10-nm CGL, the hole transient signal still shows non-dispersive properties under various applied fields, and thus the hole mobility is determined accordingly. Only 1-μm NPB is required for determining the electron mobility by using the proposed CGL. Both the thicknesses are the thinnest value reported to data. In addition, the flexibility of fabrication process of small molecules can deposit the proposed CGL underneath and atop the material under test. Therefore, this technique is applicable to small-molecule and polymeric materials. We also propose a new approach to design the TOF sample using an optical simulation. These results strongly demonstrate that the proposed technique is valuable tool in determining the carrier mobility and may spur additional research in this field. |
format | Online Article Text |
id | pubmed-4441200 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2015 |
publisher | Nature Publishing Group |
record_format | MEDLINE/PubMed |
spelling | pubmed-44412002015-05-29 Downscaling the Sample Thickness to Sub-Micrometers by Employing Organic Photovoltaic Materials as a Charge-Generation Layer in the Time-of-Flight Measurement Liu, Shun-Wei Lee, Chih-Chien Su, Wei-Cheng Yuan, Chih-Hsien Lin, Chun-Feng Chen, Kuan-Ting Shu, Yi-Sheng Li, Ya-Ze Su, Tsung-Hao Huang, Bo-Yao Chang, Wen-Chang Liu, Yu-Hsuan Sci Rep Article Time-of-flight (TOF) measurements typically require a sample thickness of several micrometers for determining the carrier mobility, thus rendering the applicability inefficient and unreliable because the sample thicknesses are orders of magnitude higher than those in real optoelectronic devices. Here, we use subphthalocyanine (SubPc):C(70) as a charge-generation layer (CGL) in the TOF measurement and a commonly hole-transporting layer, N,N’-diphenyl-N,N’-bis(1,1’-biphenyl)-4,4’-diamine (NPB), as a standard material under test. When the NPB thickness is reduced from 2 to 0.3 μm and with a thin 10-nm CGL, the hole transient signal still shows non-dispersive properties under various applied fields, and thus the hole mobility is determined accordingly. Only 1-μm NPB is required for determining the electron mobility by using the proposed CGL. Both the thicknesses are the thinnest value reported to data. In addition, the flexibility of fabrication process of small molecules can deposit the proposed CGL underneath and atop the material under test. Therefore, this technique is applicable to small-molecule and polymeric materials. We also propose a new approach to design the TOF sample using an optical simulation. These results strongly demonstrate that the proposed technique is valuable tool in determining the carrier mobility and may spur additional research in this field. Nature Publishing Group 2015-05-22 /pmc/articles/PMC4441200/ /pubmed/25999238 http://dx.doi.org/10.1038/srep10384 Text en Copyright © 2015, Macmillan Publishers Limited http://creativecommons.org/licenses/by/4.0/ This work is licensed under a Creative Commons Attribution 4.0 International License. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in the credit line; if the material is not included under the Creative Commons license, users will need to obtain permission from the license holder to reproduce the material. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/ |
spellingShingle | Article Liu, Shun-Wei Lee, Chih-Chien Su, Wei-Cheng Yuan, Chih-Hsien Lin, Chun-Feng Chen, Kuan-Ting Shu, Yi-Sheng Li, Ya-Ze Su, Tsung-Hao Huang, Bo-Yao Chang, Wen-Chang Liu, Yu-Hsuan Downscaling the Sample Thickness to Sub-Micrometers by Employing Organic Photovoltaic Materials as a Charge-Generation Layer in the Time-of-Flight Measurement |
title | Downscaling the Sample Thickness to Sub-Micrometers by Employing Organic Photovoltaic
Materials as a Charge-Generation Layer in the Time-of-Flight Measurement |
title_full | Downscaling the Sample Thickness to Sub-Micrometers by Employing Organic Photovoltaic
Materials as a Charge-Generation Layer in the Time-of-Flight Measurement |
title_fullStr | Downscaling the Sample Thickness to Sub-Micrometers by Employing Organic Photovoltaic
Materials as a Charge-Generation Layer in the Time-of-Flight Measurement |
title_full_unstemmed | Downscaling the Sample Thickness to Sub-Micrometers by Employing Organic Photovoltaic
Materials as a Charge-Generation Layer in the Time-of-Flight Measurement |
title_short | Downscaling the Sample Thickness to Sub-Micrometers by Employing Organic Photovoltaic
Materials as a Charge-Generation Layer in the Time-of-Flight Measurement |
title_sort | downscaling the sample thickness to sub-micrometers by employing organic photovoltaic
materials as a charge-generation layer in the time-of-flight measurement |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4441200/ https://www.ncbi.nlm.nih.gov/pubmed/25999238 http://dx.doi.org/10.1038/srep10384 |
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