Characterizations of photoconductivity of graphene oxide thin films

Characterizations of photoresponse of a graphene oxide (GO) thin film to a near infrared laser light were studied. Results showed the photocurrent in the GO thin film was cathodic, always flowing in an opposite direction to the initial current generated by the preset bias voltage that shows a fundam...

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Main Authors: Shiang-Kuo Chang-Jian, Jeng-Rong Ho, J.-W. John Cheng, Ya-Ping Hsieh
Format: Article
Language:English
Published: AIP Publishing LLC 2012-06-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/1.3702871
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spelling doaj-1ad661f28e414f2480288b0849311e942020-11-25T00:10:19ZengAIP Publishing LLCAIP Advances2158-32262012-06-0122022104022104-910.1063/1.3702871004202ADVCharacterizations of photoconductivity of graphene oxide thin filmsShiang-Kuo Chang-Jian0Jeng-Rong Ho1J.-W. John Cheng2Ya-Ping Hsieh3Department of Mechanical Engineering, National Chung Cheng University, Chia-Yi, 621, TaiwanDepartment of Mechanical Engineering, National Central University, Jhongli, 320, TaiwanDepartment of Mechanical Engineering, National Chung Cheng University, Chia-Yi, 621, TaiwanGraduate Institute of Optomechatronics, National Chung Cheng University, Chia-Yi, 621, TaiwanCharacterizations of photoresponse of a graphene oxide (GO) thin film to a near infrared laser light were studied. Results showed the photocurrent in the GO thin film was cathodic, always flowing in an opposite direction to the initial current generated by the preset bias voltage that shows a fundamental discrepancy from the photocurrent in the reduced graphene oxide thin film. Light illumination on the GO thin film thus results in more free electrons that offset the initial current. By examining GO thin films reduced at different temperatures, the critical temperature for reversing the photocurrent from cathodic to anodic was found around 187°C. The dynamic photoresponse for the GO thin film was further characterized through the response time constants within the laser on and off durations, denoted as τon and τoff, respectively. τon for the GO thin film was comparable to the other carbon-based thin films such as carbon nanotubes and graphenes. τoff was, however, much larger than that of the other's. This discrepancy was attributable to the retardation of exciton recombination rate thanks to the existing oxygen functional groups and defects in the GO thin films.http://dx.doi.org/10.1063/1.3702871
collection DOAJ
language English
format Article
sources DOAJ
author Shiang-Kuo Chang-Jian
Jeng-Rong Ho
J.-W. John Cheng
Ya-Ping Hsieh
spellingShingle Shiang-Kuo Chang-Jian
Jeng-Rong Ho
J.-W. John Cheng
Ya-Ping Hsieh
Characterizations of photoconductivity of graphene oxide thin films
AIP Advances
author_facet Shiang-Kuo Chang-Jian
Jeng-Rong Ho
J.-W. John Cheng
Ya-Ping Hsieh
author_sort Shiang-Kuo Chang-Jian
title Characterizations of photoconductivity of graphene oxide thin films
title_short Characterizations of photoconductivity of graphene oxide thin films
title_full Characterizations of photoconductivity of graphene oxide thin films
title_fullStr Characterizations of photoconductivity of graphene oxide thin films
title_full_unstemmed Characterizations of photoconductivity of graphene oxide thin films
title_sort characterizations of photoconductivity of graphene oxide thin films
publisher AIP Publishing LLC
series AIP Advances
issn 2158-3226
publishDate 2012-06-01
description Characterizations of photoresponse of a graphene oxide (GO) thin film to a near infrared laser light were studied. Results showed the photocurrent in the GO thin film was cathodic, always flowing in an opposite direction to the initial current generated by the preset bias voltage that shows a fundamental discrepancy from the photocurrent in the reduced graphene oxide thin film. Light illumination on the GO thin film thus results in more free electrons that offset the initial current. By examining GO thin films reduced at different temperatures, the critical temperature for reversing the photocurrent from cathodic to anodic was found around 187°C. The dynamic photoresponse for the GO thin film was further characterized through the response time constants within the laser on and off durations, denoted as τon and τoff, respectively. τon for the GO thin film was comparable to the other carbon-based thin films such as carbon nanotubes and graphenes. τoff was, however, much larger than that of the other's. This discrepancy was attributable to the retardation of exciton recombination rate thanks to the existing oxygen functional groups and defects in the GO thin films.
url http://dx.doi.org/10.1063/1.3702871
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