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Sb(2)S(3) Thickness-Related Photocurrent and Optoelectronic Processes in TiO(2)/Sb(2)S(3)/P3HT Planar Hybrid Solar Cells

In this work, a comprehensive understanding of the relationship of photon absorption, internal electrical field, transport path, and relative kinetics on Sb(2)S(3) photovoltaic performance has been investigated. The n-i-p planar structure for TiO(2)/Sb(2)S(3)/P3HT heterojunction hybrid solar cells w...

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Autores principales: Wu, Fan, Pathak, Rajesh, Jiang, Lan, Chen, Weimin, Chen, Chong, Tong, Yanhua, Zhang, Tiansheng, Jian, Ronghua, Qiao, Qiquan
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Springer US 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6795671/
https://www.ncbi.nlm.nih.gov/pubmed/31620919
http://dx.doi.org/10.1186/s11671-019-3157-x
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author Wu, Fan
Pathak, Rajesh
Jiang, Lan
Chen, Weimin
Chen, Chong
Tong, Yanhua
Zhang, Tiansheng
Jian, Ronghua
Qiao, Qiquan
author_facet Wu, Fan
Pathak, Rajesh
Jiang, Lan
Chen, Weimin
Chen, Chong
Tong, Yanhua
Zhang, Tiansheng
Jian, Ronghua
Qiao, Qiquan
author_sort Wu, Fan
collection PubMed
description In this work, a comprehensive understanding of the relationship of photon absorption, internal electrical field, transport path, and relative kinetics on Sb(2)S(3) photovoltaic performance has been investigated. The n-i-p planar structure for TiO(2)/Sb(2)S(3)/P3HT heterojunction hybrid solar cells was conducted, and the photon-to-electron processes including illumination depth, internal electric field, drift velocity and kinetic energy of charges, photo-generated electrons and hole concentration-related surface potential in Sb(2)S(3), charge transport time, and interfacial charge recombination lifetime were studied to reveal the key factors that governed the device photocurrent. Dark J–V curves, Kelvin probe force microscope, and intensity-modulated photocurrent/photovoltage dynamics indicate that internal electric field is the main factors that affect the photocurrent when the Sb(2)S(3) thickness is less than the hole diffusion length. However, when the Sb(2)S(3) thickness is larger than the hole diffusion length, the inferior area in Sb(2)S(3) for holes that cannot be diffused to P3HT would become a dominant factor affecting the photocurrent. The inferior area in Sb(2)S(3) layer for hole collection could also affect the V(oc) of the device. The reduced collection of holes in P3HT, when the Sb(2)S(3) thickness is larger than the hole diffusion length, would increase the difference between the quasi-Fermi levels of electrons and holes for a lower V(oc).
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spelling pubmed-67956712019-10-24 Sb(2)S(3) Thickness-Related Photocurrent and Optoelectronic Processes in TiO(2)/Sb(2)S(3)/P3HT Planar Hybrid Solar Cells Wu, Fan Pathak, Rajesh Jiang, Lan Chen, Weimin Chen, Chong Tong, Yanhua Zhang, Tiansheng Jian, Ronghua Qiao, Qiquan Nanoscale Res Lett Nano Express In this work, a comprehensive understanding of the relationship of photon absorption, internal electrical field, transport path, and relative kinetics on Sb(2)S(3) photovoltaic performance has been investigated. The n-i-p planar structure for TiO(2)/Sb(2)S(3)/P3HT heterojunction hybrid solar cells was conducted, and the photon-to-electron processes including illumination depth, internal electric field, drift velocity and kinetic energy of charges, photo-generated electrons and hole concentration-related surface potential in Sb(2)S(3), charge transport time, and interfacial charge recombination lifetime were studied to reveal the key factors that governed the device photocurrent. Dark J–V curves, Kelvin probe force microscope, and intensity-modulated photocurrent/photovoltage dynamics indicate that internal electric field is the main factors that affect the photocurrent when the Sb(2)S(3) thickness is less than the hole diffusion length. However, when the Sb(2)S(3) thickness is larger than the hole diffusion length, the inferior area in Sb(2)S(3) for holes that cannot be diffused to P3HT would become a dominant factor affecting the photocurrent. The inferior area in Sb(2)S(3) layer for hole collection could also affect the V(oc) of the device. The reduced collection of holes in P3HT, when the Sb(2)S(3) thickness is larger than the hole diffusion length, would increase the difference between the quasi-Fermi levels of electrons and holes for a lower V(oc). Springer US 2019-10-16 /pmc/articles/PMC6795671/ /pubmed/31620919 http://dx.doi.org/10.1186/s11671-019-3157-x Text en © The Author(s). 2019 Open AccessThis article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.
spellingShingle Nano Express
Wu, Fan
Pathak, Rajesh
Jiang, Lan
Chen, Weimin
Chen, Chong
Tong, Yanhua
Zhang, Tiansheng
Jian, Ronghua
Qiao, Qiquan
Sb(2)S(3) Thickness-Related Photocurrent and Optoelectronic Processes in TiO(2)/Sb(2)S(3)/P3HT Planar Hybrid Solar Cells
title Sb(2)S(3) Thickness-Related Photocurrent and Optoelectronic Processes in TiO(2)/Sb(2)S(3)/P3HT Planar Hybrid Solar Cells
title_full Sb(2)S(3) Thickness-Related Photocurrent and Optoelectronic Processes in TiO(2)/Sb(2)S(3)/P3HT Planar Hybrid Solar Cells
title_fullStr Sb(2)S(3) Thickness-Related Photocurrent and Optoelectronic Processes in TiO(2)/Sb(2)S(3)/P3HT Planar Hybrid Solar Cells
title_full_unstemmed Sb(2)S(3) Thickness-Related Photocurrent and Optoelectronic Processes in TiO(2)/Sb(2)S(3)/P3HT Planar Hybrid Solar Cells
title_short Sb(2)S(3) Thickness-Related Photocurrent and Optoelectronic Processes in TiO(2)/Sb(2)S(3)/P3HT Planar Hybrid Solar Cells
title_sort sb(2)s(3) thickness-related photocurrent and optoelectronic processes in tio(2)/sb(2)s(3)/p3ht planar hybrid solar cells
topic Nano Express
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6795671/
https://www.ncbi.nlm.nih.gov/pubmed/31620919
http://dx.doi.org/10.1186/s11671-019-3157-x
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