Numerical Simulation of Nitrogen-Doped Titanium Dioxide as an Inorganic Hole Transport Layer in Mixed Halide Perovskite Structures Using SCAPS 1-D

Perovskite solar cells (PSCs) stand out as superior third-generation (III-gen) thin-film energy harvesting structures with high efficiency, optical properties and light transmission ability. However, the need to develop cost-effective, stable and sustainable PSCs is allied to the influence of the ab...

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Main Authors: Nitin Ralph Pochont, Yendaluru Raja Sekhar
Format: Article
Language:English
Published: MDPI AG 2022-12-01
Series:Inorganics
Subjects:
Online Access:https://www.mdpi.com/2304-6740/11/1/3
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author Nitin Ralph Pochont
Yendaluru Raja Sekhar
author_facet Nitin Ralph Pochont
Yendaluru Raja Sekhar
author_sort Nitin Ralph Pochont
collection DOAJ
description Perovskite solar cells (PSCs) stand out as superior third-generation (III-gen) thin-film energy harvesting structures with high efficiency, optical properties and light transmission ability. However, the need to develop cost-effective, stable and sustainable PSCs is allied to the influence of the absorber layer and charge selective transport layers when achieving semi-transparent (ST) structures. Using SCAPS simulation software that can envisage the conceptuality in devising ST PSCs, this work explores and reports the electrical performance of different methylammonium (MA)-based perovskite structures (FTO/TiO<sub>2</sub>/PCBM/SnO<sub>2</sub>/MAPbI<sub>3</sub>/TiO<sub>2</sub>:N/PTAA/Spiro-OMeTAD/PEDOT: PSS/Ag). The influence of absorber thickness and defect density is analyzed with optimal parameters. This research reports a novel idea that replaces the polymeric hole transport layer (HTL), such as Spiro-OMeTAD, PEDOT: PSS and PTAA with an air-stable inorganic metal oxide, viz., nitrogen-doped titanium dioxide (TiO<sub>2</sub>:N). The simulation results depict an attainable power conversion efficiency of 9.92%, 10.11% and 11.54% for the proposed structures with the novel HTL that are on par with polymeric HTLs. Furthermore, the maximum allowable absorber thickness was 600 nm with a threshold defect density of 1 × 10<sup>15</sup> cm<sup>−3</sup>. The optimized electrical parameters can be implemented to develop thin-film light transmission perovskite cells with rational power conversion efficiencies.
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spelling doaj.art-4f06e3318eb34019a3cdd0c3ab90cf5c2023-11-30T22:46:56ZengMDPI AGInorganics2304-67402022-12-01111310.3390/inorganics11010003Numerical Simulation of Nitrogen-Doped Titanium Dioxide as an Inorganic Hole Transport Layer in Mixed Halide Perovskite Structures Using SCAPS 1-DNitin Ralph Pochont0Yendaluru Raja Sekhar1School of Mechanical Engineering, Vellore Institute of Technology, Vellore 632014, IndiaCentre for Disaster Mitigation and Management, Vellore Institute of Technology, Vellore 632014, IndiaPerovskite solar cells (PSCs) stand out as superior third-generation (III-gen) thin-film energy harvesting structures with high efficiency, optical properties and light transmission ability. However, the need to develop cost-effective, stable and sustainable PSCs is allied to the influence of the absorber layer and charge selective transport layers when achieving semi-transparent (ST) structures. Using SCAPS simulation software that can envisage the conceptuality in devising ST PSCs, this work explores and reports the electrical performance of different methylammonium (MA)-based perovskite structures (FTO/TiO<sub>2</sub>/PCBM/SnO<sub>2</sub>/MAPbI<sub>3</sub>/TiO<sub>2</sub>:N/PTAA/Spiro-OMeTAD/PEDOT: PSS/Ag). The influence of absorber thickness and defect density is analyzed with optimal parameters. This research reports a novel idea that replaces the polymeric hole transport layer (HTL), such as Spiro-OMeTAD, PEDOT: PSS and PTAA with an air-stable inorganic metal oxide, viz., nitrogen-doped titanium dioxide (TiO<sub>2</sub>:N). The simulation results depict an attainable power conversion efficiency of 9.92%, 10.11% and 11.54% for the proposed structures with the novel HTL that are on par with polymeric HTLs. Furthermore, the maximum allowable absorber thickness was 600 nm with a threshold defect density of 1 × 10<sup>15</sup> cm<sup>−3</sup>. The optimized electrical parameters can be implemented to develop thin-film light transmission perovskite cells with rational power conversion efficiencies.https://www.mdpi.com/2304-6740/11/1/3nitrogen-doped titanium dioxideinorganic layerabsorber thicknessdefect densityelectrical parametersSCAPS simulation
spellingShingle Nitin Ralph Pochont
Yendaluru Raja Sekhar
Numerical Simulation of Nitrogen-Doped Titanium Dioxide as an Inorganic Hole Transport Layer in Mixed Halide Perovskite Structures Using SCAPS 1-D
Inorganics
nitrogen-doped titanium dioxide
inorganic layer
absorber thickness
defect density
electrical parameters
SCAPS simulation
title Numerical Simulation of Nitrogen-Doped Titanium Dioxide as an Inorganic Hole Transport Layer in Mixed Halide Perovskite Structures Using SCAPS 1-D
title_full Numerical Simulation of Nitrogen-Doped Titanium Dioxide as an Inorganic Hole Transport Layer in Mixed Halide Perovskite Structures Using SCAPS 1-D
title_fullStr Numerical Simulation of Nitrogen-Doped Titanium Dioxide as an Inorganic Hole Transport Layer in Mixed Halide Perovskite Structures Using SCAPS 1-D
title_full_unstemmed Numerical Simulation of Nitrogen-Doped Titanium Dioxide as an Inorganic Hole Transport Layer in Mixed Halide Perovskite Structures Using SCAPS 1-D
title_short Numerical Simulation of Nitrogen-Doped Titanium Dioxide as an Inorganic Hole Transport Layer in Mixed Halide Perovskite Structures Using SCAPS 1-D
title_sort numerical simulation of nitrogen doped titanium dioxide as an inorganic hole transport layer in mixed halide perovskite structures using scaps 1 d
topic nitrogen-doped titanium dioxide
inorganic layer
absorber thickness
defect density
electrical parameters
SCAPS simulation
url https://www.mdpi.com/2304-6740/11/1/3
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