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Electrically Enhanced Transition Metal Dichalcogenides as Charge Transport Layers in Metallophthalocyanine-Based Solar Cells

Transitional metal dichalcogenides (TMDs), such as molybdenum disulfide (MoS(2)) have found application in photovoltaic cells as a charge transporting layer due to their high carrier mobility, chemical stability, and flexibility. In this research, a photovoltaic device was fabricated consisting of c...

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Autores principales: Manamela, Lebogang, Fru, Juvet N., Kyesmen, Pannan I., Diale, Mmantsae, Nombona, Nolwazi
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Frontiers Media S.A. 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7746773/
https://www.ncbi.nlm.nih.gov/pubmed/33344424
http://dx.doi.org/10.3389/fchem.2020.612418
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author Manamela, Lebogang
Fru, Juvet N.
Kyesmen, Pannan I.
Diale, Mmantsae
Nombona, Nolwazi
author_facet Manamela, Lebogang
Fru, Juvet N.
Kyesmen, Pannan I.
Diale, Mmantsae
Nombona, Nolwazi
author_sort Manamela, Lebogang
collection PubMed
description Transitional metal dichalcogenides (TMDs), such as molybdenum disulfide (MoS(2)) have found application in photovoltaic cells as a charge transporting layer due to their high carrier mobility, chemical stability, and flexibility. In this research, a photovoltaic device was fabricated consisting of copper phthalocyanine (CuPc) as the active layer, exfoliated and Au-doped MoS(2), which are n-type and p-type as electron and hole transport layers, respectively. XRD studies showed prominent peaks at (002) and other weak reflections at (100), (103), (006), and (105) planes corresponding to those of bulky MoS(2). The only maintained reflection at (002) was weakened for the exfoliated MoS(2) compared to the bulk, which confirmed that the material was highly exfoliated. Additional peaks at (111) and (200) planes were observed for the Au doped MoS(2). The interlayer spacing (d(002)) was calculated to be 0.62 nm for the trigonal prismatic MoS(2) with the space group P6m2. Raman spectroscopy showed that the [Formula: see text] g (393 cm(−1)) and A(1g) (409 cm(−1)) peaks for exfoliated MoS(2) are closer to each other compared to their bulk counterparts (378 and 408 cm(−1), respectively) hence confirming exfoliation. Raman spectroscopy also confirmed doping of MoS(2) by Au as the Au-S peak was observed at 320 cm(−1). Exfoliation was further confirmed by SEM as when moving from bulky to exfoliated MoS(2), a single nanosheet was observed. Doping was further proven by EDS, which detected Au in the sample suggesting the yield of a p-type Au-MoS(2). The fabricated device had the architecture: Glass/FTO/Au-MoS(2)/CuPc/MoS(2)/Au. A quadratic relationship between I-V was observed suggesting little rectification from the device. Illuminated I-V characterization verified that the device was sensitive and absorbed visible light. Upon illumination, the device was able to absorb photons to create electron-hole pairs and it was evident that semipermeable junctions were formed between Au-MoS(2)/CuPc and CuPc/MoS(2) as holes and electrons were extracted and separated at respective junctions generating current from light. This study indicates that the exfoliated and Au-MoS(2) could be employed as an electron transporting layer (ETL) and hole transporting layer (HTL), respectively in fabricating photovoltaic devices.
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spelling pubmed-77467732020-12-19 Electrically Enhanced Transition Metal Dichalcogenides as Charge Transport Layers in Metallophthalocyanine-Based Solar Cells Manamela, Lebogang Fru, Juvet N. Kyesmen, Pannan I. Diale, Mmantsae Nombona, Nolwazi Front Chem Chemistry Transitional metal dichalcogenides (TMDs), such as molybdenum disulfide (MoS(2)) have found application in photovoltaic cells as a charge transporting layer due to their high carrier mobility, chemical stability, and flexibility. In this research, a photovoltaic device was fabricated consisting of copper phthalocyanine (CuPc) as the active layer, exfoliated and Au-doped MoS(2), which are n-type and p-type as electron and hole transport layers, respectively. XRD studies showed prominent peaks at (002) and other weak reflections at (100), (103), (006), and (105) planes corresponding to those of bulky MoS(2). The only maintained reflection at (002) was weakened for the exfoliated MoS(2) compared to the bulk, which confirmed that the material was highly exfoliated. Additional peaks at (111) and (200) planes were observed for the Au doped MoS(2). The interlayer spacing (d(002)) was calculated to be 0.62 nm for the trigonal prismatic MoS(2) with the space group P6m2. Raman spectroscopy showed that the [Formula: see text] g (393 cm(−1)) and A(1g) (409 cm(−1)) peaks for exfoliated MoS(2) are closer to each other compared to their bulk counterparts (378 and 408 cm(−1), respectively) hence confirming exfoliation. Raman spectroscopy also confirmed doping of MoS(2) by Au as the Au-S peak was observed at 320 cm(−1). Exfoliation was further confirmed by SEM as when moving from bulky to exfoliated MoS(2), a single nanosheet was observed. Doping was further proven by EDS, which detected Au in the sample suggesting the yield of a p-type Au-MoS(2). The fabricated device had the architecture: Glass/FTO/Au-MoS(2)/CuPc/MoS(2)/Au. A quadratic relationship between I-V was observed suggesting little rectification from the device. Illuminated I-V characterization verified that the device was sensitive and absorbed visible light. Upon illumination, the device was able to absorb photons to create electron-hole pairs and it was evident that semipermeable junctions were formed between Au-MoS(2)/CuPc and CuPc/MoS(2) as holes and electrons were extracted and separated at respective junctions generating current from light. This study indicates that the exfoliated and Au-MoS(2) could be employed as an electron transporting layer (ETL) and hole transporting layer (HTL), respectively in fabricating photovoltaic devices. Frontiers Media S.A. 2020-12-04 /pmc/articles/PMC7746773/ /pubmed/33344424 http://dx.doi.org/10.3389/fchem.2020.612418 Text en Copyright © 2020 Manamela, Fru, Kyesmen, Diale and Nombona. http://creativecommons.org/licenses/by/4.0/ This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
spellingShingle Chemistry
Manamela, Lebogang
Fru, Juvet N.
Kyesmen, Pannan I.
Diale, Mmantsae
Nombona, Nolwazi
Electrically Enhanced Transition Metal Dichalcogenides as Charge Transport Layers in Metallophthalocyanine-Based Solar Cells
title Electrically Enhanced Transition Metal Dichalcogenides as Charge Transport Layers in Metallophthalocyanine-Based Solar Cells
title_full Electrically Enhanced Transition Metal Dichalcogenides as Charge Transport Layers in Metallophthalocyanine-Based Solar Cells
title_fullStr Electrically Enhanced Transition Metal Dichalcogenides as Charge Transport Layers in Metallophthalocyanine-Based Solar Cells
title_full_unstemmed Electrically Enhanced Transition Metal Dichalcogenides as Charge Transport Layers in Metallophthalocyanine-Based Solar Cells
title_short Electrically Enhanced Transition Metal Dichalcogenides as Charge Transport Layers in Metallophthalocyanine-Based Solar Cells
title_sort electrically enhanced transition metal dichalcogenides as charge transport layers in metallophthalocyanine-based solar cells
topic Chemistry
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7746773/
https://www.ncbi.nlm.nih.gov/pubmed/33344424
http://dx.doi.org/10.3389/fchem.2020.612418
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