Role of Interfacial Oxide Layer in MoOx/n-Si Heterojunction Solar Cells

Interfacial oxide layer plays a crucial role in a MoOx/n-Si heterojunction (MSHJ) solar cell; however, the nature of this interfacial layer is not yet clarified. In this study, based on the experimental results, we theoretically analyzed the role of the interfacial oxide layer in the charge carrier...

Full description

Bibliographic Details
Main Authors: X. M. Song, Z. G. Huang, M. Gao, D. Y. Chen, Z. Fan, Z. Q. Ma
Format: Article
Language:English
Published: Hindawi Limited 2021-01-01
Series:International Journal of Photoenergy
Online Access:http://dx.doi.org/10.1155/2021/6623150
id doaj-1c3e40f5f36e4626bb0d4cf0d6476cb7
record_format Article
spelling doaj-1c3e40f5f36e4626bb0d4cf0d6476cb72021-05-03T00:00:28ZengHindawi LimitedInternational Journal of Photoenergy1687-529X2021-01-01202110.1155/2021/6623150Role of Interfacial Oxide Layer in MoOx/n-Si Heterojunction Solar CellsX. M. Song0Z. G. Huang1M. Gao2D. Y. Chen3Z. Fan4Z. Q. Ma5SHU-SolarE R&D LabSchool of ScienceSHU-SolarE R&D LabSHU-SolarE R&D LabSchool of ScienceSHU-SolarE R&D LabInterfacial oxide layer plays a crucial role in a MoOx/n-Si heterojunction (MSHJ) solar cell; however, the nature of this interfacial layer is not yet clarified. In this study, based on the experimental results, we theoretically analyzed the role of the interfacial oxide layer in the charge carrier transport of the MSHJ device. The interfacial oxide layer is regarded as two layers: a quasi p-type semiconductor interfacial oxide layer (SiOx(Mo))1 in which numerous negatively charged centers existed due to oxygen vacancies and molybdenum–ion-correlated ternary hybrids and a buffer layer (SiOx(Mo))2 in which the quantity of Si-O bonds was dominated by relatively good passivation. The thickness of (SiOx(Mo))1 and the thickness of (SiOx(Mo))2 were about 2.0 nm and 1.5 nm, respectively. The simulation results revealed that the quasi p-type layer behaved as a semiconductor material with a wide band gap of 2.30 eV, facilitating the transport of holes for negatively charged centers. Additionally, the buffer layer with an optical band gap of 1.90 eV played a crucial role in passivation in the MoOx/n-Si devices. Furthermore, the negative charge centers in the interfacial layer had dual functions in both the field passivation and the tunneling processes. Combined with the experimental results, our model clarifies the interfacial physics and the mechanism of carrier transport for an MSHJ solar cell and provides an effective way to the high efficiency of MSHJ solar cells.http://dx.doi.org/10.1155/2021/6623150
collection DOAJ
language English
format Article
sources DOAJ
author X. M. Song
Z. G. Huang
M. Gao
D. Y. Chen
Z. Fan
Z. Q. Ma
spellingShingle X. M. Song
Z. G. Huang
M. Gao
D. Y. Chen
Z. Fan
Z. Q. Ma
Role of Interfacial Oxide Layer in MoOx/n-Si Heterojunction Solar Cells
International Journal of Photoenergy
author_facet X. M. Song
Z. G. Huang
M. Gao
D. Y. Chen
Z. Fan
Z. Q. Ma
author_sort X. M. Song
title Role of Interfacial Oxide Layer in MoOx/n-Si Heterojunction Solar Cells
title_short Role of Interfacial Oxide Layer in MoOx/n-Si Heterojunction Solar Cells
title_full Role of Interfacial Oxide Layer in MoOx/n-Si Heterojunction Solar Cells
title_fullStr Role of Interfacial Oxide Layer in MoOx/n-Si Heterojunction Solar Cells
title_full_unstemmed Role of Interfacial Oxide Layer in MoOx/n-Si Heterojunction Solar Cells
title_sort role of interfacial oxide layer in moox/n-si heterojunction solar cells
publisher Hindawi Limited
series International Journal of Photoenergy
issn 1687-529X
publishDate 2021-01-01
description Interfacial oxide layer plays a crucial role in a MoOx/n-Si heterojunction (MSHJ) solar cell; however, the nature of this interfacial layer is not yet clarified. In this study, based on the experimental results, we theoretically analyzed the role of the interfacial oxide layer in the charge carrier transport of the MSHJ device. The interfacial oxide layer is regarded as two layers: a quasi p-type semiconductor interfacial oxide layer (SiOx(Mo))1 in which numerous negatively charged centers existed due to oxygen vacancies and molybdenum–ion-correlated ternary hybrids and a buffer layer (SiOx(Mo))2 in which the quantity of Si-O bonds was dominated by relatively good passivation. The thickness of (SiOx(Mo))1 and the thickness of (SiOx(Mo))2 were about 2.0 nm and 1.5 nm, respectively. The simulation results revealed that the quasi p-type layer behaved as a semiconductor material with a wide band gap of 2.30 eV, facilitating the transport of holes for negatively charged centers. Additionally, the buffer layer with an optical band gap of 1.90 eV played a crucial role in passivation in the MoOx/n-Si devices. Furthermore, the negative charge centers in the interfacial layer had dual functions in both the field passivation and the tunneling processes. Combined with the experimental results, our model clarifies the interfacial physics and the mechanism of carrier transport for an MSHJ solar cell and provides an effective way to the high efficiency of MSHJ solar cells.
url http://dx.doi.org/10.1155/2021/6623150
work_keys_str_mv AT xmsong roleofinterfacialoxidelayerinmooxnsiheterojunctionsolarcells
AT zghuang roleofinterfacialoxidelayerinmooxnsiheterojunctionsolarcells
AT mgao roleofinterfacialoxidelayerinmooxnsiheterojunctionsolarcells
AT dychen roleofinterfacialoxidelayerinmooxnsiheterojunctionsolarcells
AT zfan roleofinterfacialoxidelayerinmooxnsiheterojunctionsolarcells
AT zqma roleofinterfacialoxidelayerinmooxnsiheterojunctionsolarcells
_version_ 1714634999454498816