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Power Factor of One Molecule Thick Films and Length Dependence
[Image: see text] There is a rapidly increasing interest in organic thin film thermoelectrics. However, the power factor of one molecule thick organic film, the self-assembled monolayer (SAM), has not yet been determined. This study describes the experimental determination of the power factor in SAM...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical
Society
2019
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6936095/ https://www.ncbi.nlm.nih.gov/pubmed/31893227 http://dx.doi.org/10.1021/acscentsci.9b01042 |
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author | Park, Sohyun Kang, Seohyun Yoon, Hyo Jae |
author_facet | Park, Sohyun Kang, Seohyun Yoon, Hyo Jae |
author_sort | Park, Sohyun |
collection | PubMed |
description | [Image: see text] There is a rapidly increasing interest in organic thin film thermoelectrics. However, the power factor of one molecule thick organic film, the self-assembled monolayer (SAM), has not yet been determined. This study describes the experimental determination of the power factor in SAMs and its length dependence at an atomic level. As a proof-of-concept, SAMs composed of n-alkanethiolates and oligophenylenethiolates of different lengths are focused. These SAMs were electrically and thermoelectrically characterized on an identical junction platform using a liquid metal top-electrode, allowing the straightforward estimation of the power factor of the monolayers. The results show that the power factor of the alkyl SAMs ranged from 2.0 × 10(–8) to 8.0 × 10(–12) μW m(–1) K(–2) and exhibited significant negative length dependence, whereas the conductivity and thermopower of the conjugated SAMs are the two opposing factors that balance the power factor upon an increase in molecular length, exhibiting a maximum power factor of 3.6 × 10(–8) μW m(–1) K(–2). Once correction factors about the ratio of effective contact area to geometrical contact area are considered, the values of power factors can be increased by several orders of magnitude. With a newly derived parametric semiempirical model describing the length dependence of the power factor, it is investigated that one molecule thick films thinner than 10 nm composed of thiophene units can yield power factors rivaling those of famed organic thermoelectric materials based on poly(3,4-ethylenedioxythiophene)/polystyrenesulfonate (PEDOT/PSS) and polyaniline/graphene/double-walled carbon nanotube. Furthermore, how the transition of the transport regime from tunneling to hopping as molecules become long affects power factors is examined. |
format | Online Article Text |
id | pubmed-6936095 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2019 |
publisher | American Chemical
Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-69360952019-12-31 Power Factor of One Molecule Thick Films and Length Dependence Park, Sohyun Kang, Seohyun Yoon, Hyo Jae ACS Cent Sci [Image: see text] There is a rapidly increasing interest in organic thin film thermoelectrics. However, the power factor of one molecule thick organic film, the self-assembled monolayer (SAM), has not yet been determined. This study describes the experimental determination of the power factor in SAMs and its length dependence at an atomic level. As a proof-of-concept, SAMs composed of n-alkanethiolates and oligophenylenethiolates of different lengths are focused. These SAMs were electrically and thermoelectrically characterized on an identical junction platform using a liquid metal top-electrode, allowing the straightforward estimation of the power factor of the monolayers. The results show that the power factor of the alkyl SAMs ranged from 2.0 × 10(–8) to 8.0 × 10(–12) μW m(–1) K(–2) and exhibited significant negative length dependence, whereas the conductivity and thermopower of the conjugated SAMs are the two opposing factors that balance the power factor upon an increase in molecular length, exhibiting a maximum power factor of 3.6 × 10(–8) μW m(–1) K(–2). Once correction factors about the ratio of effective contact area to geometrical contact area are considered, the values of power factors can be increased by several orders of magnitude. With a newly derived parametric semiempirical model describing the length dependence of the power factor, it is investigated that one molecule thick films thinner than 10 nm composed of thiophene units can yield power factors rivaling those of famed organic thermoelectric materials based on poly(3,4-ethylenedioxythiophene)/polystyrenesulfonate (PEDOT/PSS) and polyaniline/graphene/double-walled carbon nanotube. Furthermore, how the transition of the transport regime from tunneling to hopping as molecules become long affects power factors is examined. American Chemical Society 2019-12-05 2019-12-26 /pmc/articles/PMC6936095/ /pubmed/31893227 http://dx.doi.org/10.1021/acscentsci.9b01042 Text en Copyright © 2019 American Chemical Society This is an open access article published under an ACS AuthorChoice License (http://pubs.acs.org/page/policy/authorchoice_termsofuse.html) , which permits copying and redistribution of the article or any adaptations for non-commercial purposes. |
spellingShingle | Park, Sohyun Kang, Seohyun Yoon, Hyo Jae Power Factor of One Molecule Thick Films and Length Dependence |
title | Power Factor
of One Molecule Thick Films and Length
Dependence |
title_full | Power Factor
of One Molecule Thick Films and Length
Dependence |
title_fullStr | Power Factor
of One Molecule Thick Films and Length
Dependence |
title_full_unstemmed | Power Factor
of One Molecule Thick Films and Length
Dependence |
title_short | Power Factor
of One Molecule Thick Films and Length
Dependence |
title_sort | power factor
of one molecule thick films and length
dependence |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6936095/ https://www.ncbi.nlm.nih.gov/pubmed/31893227 http://dx.doi.org/10.1021/acscentsci.9b01042 |
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