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Engineering of ZnO/rGO towards NO(2) Gas Detection: Ratio Modulated Sensing Type and Heterojunction Determined Response

Nanoscale heterostructured zinc oxide/reduced graphene oxide (ZnO/rGO) materials with p–n heterojunctions exhibit excellent low temperature NO(2) gas sensing performance, but their doping ratio modulated sensing properties remain poorly understood. Herein, ZnO nanoparticles were loaded with 0.1~4% r...

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Detalles Bibliográficos
Autores principales: Li, Donglin, Lu, Junfeng, Zhang, Xuanji, Jin, Dingfeng, Jin, Hongxiao
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10004851/
https://www.ncbi.nlm.nih.gov/pubmed/36903795
http://dx.doi.org/10.3390/nano13050917
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author Li, Donglin
Lu, Junfeng
Zhang, Xuanji
Jin, Dingfeng
Jin, Hongxiao
author_facet Li, Donglin
Lu, Junfeng
Zhang, Xuanji
Jin, Dingfeng
Jin, Hongxiao
author_sort Li, Donglin
collection PubMed
description Nanoscale heterostructured zinc oxide/reduced graphene oxide (ZnO/rGO) materials with p–n heterojunctions exhibit excellent low temperature NO(2) gas sensing performance, but their doping ratio modulated sensing properties remain poorly understood. Herein, ZnO nanoparticles were loaded with 0.1~4% rGO by a facile hydrothermal method and evaluated as NO(2) gas chemiresistor. We have the following key findings. First, ZnO/rGO manifests doping ratio-dependent sensing type switching. Increasing the rGO concentration changes the type of ZnO/rGO conductivity from n-type (<0.6% rGO) to mixed n/p -type (0.6~1.4% rGO) and finally to p-type (>1.4% rGO). Second, interestingly, different sensing regions exhibit different sensing characteristics. In the n-type NO(2) gas sensing region, all the sensors exhibit the maximum gas response at the optimum working temperature. Among them, the sensor that shows the maximum gas response exhibits a minimum optimum working temperature. In the mixed n/p-type region, the material displays abnormal reversal from n- to p-type sensing transitions as a function of the doping ratio, NO(2) concentration and working temperature. In the p-type gas sensing region, the response decreases with increasing rGO ratio and working temperature. Third, we derive a conduction path model that shows how the sensing type switches in ZnO/rGO. We also find that p–n heterojunction ratio (n(p–n)/n(rGO)) plays a key role in the optimal response condition. The model is supported by UV-vis experimental data. The approach presented in this work can be extended to other p–n heterostructures and the insights will benefit the design of more efficient chemiresistive gas sensors.
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spelling pubmed-100048512023-03-11 Engineering of ZnO/rGO towards NO(2) Gas Detection: Ratio Modulated Sensing Type and Heterojunction Determined Response Li, Donglin Lu, Junfeng Zhang, Xuanji Jin, Dingfeng Jin, Hongxiao Nanomaterials (Basel) Article Nanoscale heterostructured zinc oxide/reduced graphene oxide (ZnO/rGO) materials with p–n heterojunctions exhibit excellent low temperature NO(2) gas sensing performance, but their doping ratio modulated sensing properties remain poorly understood. Herein, ZnO nanoparticles were loaded with 0.1~4% rGO by a facile hydrothermal method and evaluated as NO(2) gas chemiresistor. We have the following key findings. First, ZnO/rGO manifests doping ratio-dependent sensing type switching. Increasing the rGO concentration changes the type of ZnO/rGO conductivity from n-type (<0.6% rGO) to mixed n/p -type (0.6~1.4% rGO) and finally to p-type (>1.4% rGO). Second, interestingly, different sensing regions exhibit different sensing characteristics. In the n-type NO(2) gas sensing region, all the sensors exhibit the maximum gas response at the optimum working temperature. Among them, the sensor that shows the maximum gas response exhibits a minimum optimum working temperature. In the mixed n/p-type region, the material displays abnormal reversal from n- to p-type sensing transitions as a function of the doping ratio, NO(2) concentration and working temperature. In the p-type gas sensing region, the response decreases with increasing rGO ratio and working temperature. Third, we derive a conduction path model that shows how the sensing type switches in ZnO/rGO. We also find that p–n heterojunction ratio (n(p–n)/n(rGO)) plays a key role in the optimal response condition. The model is supported by UV-vis experimental data. The approach presented in this work can be extended to other p–n heterostructures and the insights will benefit the design of more efficient chemiresistive gas sensors. MDPI 2023-03-01 /pmc/articles/PMC10004851/ /pubmed/36903795 http://dx.doi.org/10.3390/nano13050917 Text en © 2023 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Li, Donglin
Lu, Junfeng
Zhang, Xuanji
Jin, Dingfeng
Jin, Hongxiao
Engineering of ZnO/rGO towards NO(2) Gas Detection: Ratio Modulated Sensing Type and Heterojunction Determined Response
title Engineering of ZnO/rGO towards NO(2) Gas Detection: Ratio Modulated Sensing Type and Heterojunction Determined Response
title_full Engineering of ZnO/rGO towards NO(2) Gas Detection: Ratio Modulated Sensing Type and Heterojunction Determined Response
title_fullStr Engineering of ZnO/rGO towards NO(2) Gas Detection: Ratio Modulated Sensing Type and Heterojunction Determined Response
title_full_unstemmed Engineering of ZnO/rGO towards NO(2) Gas Detection: Ratio Modulated Sensing Type and Heterojunction Determined Response
title_short Engineering of ZnO/rGO towards NO(2) Gas Detection: Ratio Modulated Sensing Type and Heterojunction Determined Response
title_sort engineering of zno/rgo towards no(2) gas detection: ratio modulated sensing type and heterojunction determined response
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10004851/
https://www.ncbi.nlm.nih.gov/pubmed/36903795
http://dx.doi.org/10.3390/nano13050917
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