Affiliations 

  • 1 Department of Materials Science and Engineering, Cornell University, Ithaca, NY, 14850, USA
  • 2 University of Warith Al-Anbiyaa, 56001, Karbala, Iraq. mustafa_kareem@yahoo.com
  • 3 Electrical Engineering Department, College of Engineering, Al-Iraqia University, Baghdad, 10011, Iraq
  • 4 Solar Lab, GLA University, Mathura, 281406, India
  • 5 Technical College of Engineering, Al-Bayan University, Baghdad, 10011, Iraq
  • 6 Faculty of Data Science & Information Technology, INTI International University, Persiaran Perdana BBN, 71800, Nilai, Negeri Sembilan, Malaysia. joseph.ng@newinti.edu.my
  • 7 Applied Sciences Department, University of Technology-Iraq, Baghdad, 10011, Iraq
  • 8 VLSI Centre of Excellence, Chitkara University Institute of Engineering and Technology, Chitkara University, Rajpura, Punjab, 140417, India
  • 9 Civil and Environmental Engineering Department, King Fahd University of Petroleum & Minerals, Dhahran, 31261, Saudi Arabia
  • 10 Institute of Electronics. Atomic Energy Research Establishment, Bangladesh Atomic Energy Commission, Dhaka, 1349, Bangladesh
Sci Rep, 2023 Jun 05;13(1):9076.
PMID: 37277466 DOI: 10.1038/s41598-023-36427-3

Abstract

According to recent reports, planar structure-based organometallic perovskite solar cells (OPSCs) have achieved remarkable power conversion efficiency (PCE), making them very competitive with the more traditional silicon photovoltaics. A complete understanding of OPSCs and their individual parts is still necessary for further enhancement in PCE. In this work, indium sulfide (In2S3)-based planar heterojunction OPSCs were proposed and simulated with the SCAPS (a Solar Cell Capacitance Simulator)-1D programme. Initially, OPSC performance was calibrated with the experimentally fabricated architecture (FTO/In2S3/MAPbI3/Spiro-OMeTAD/Au) to evaluate the optimum parameters of each layer. The numerical calculations showed a significant dependence of PCE on the thickness and defect density of the MAPbI3 absorber material. The results showed that as the perovskite layer thickness increased, the PCE improved gradually but subsequently reached a maximum at thicknesses greater than 500 nm. Moreover, parameters involving the series resistance as well as the shunt resistance were recognized to affect the performance of the OPSC. Most importantly, a champion PCE of over 20% was yielded under the optimistic simulation conditions. Overall, the OPSC performed better between 20 and 30 °C, and its efficiency rapidly decreases above that temperature.

* Title and MeSH Headings from MEDLINE®/PubMed®, a database of the U.S. National Library of Medicine.