{"title":"Computational modeling of a Sb2S3 /CdxSb2-x(S1-ySey)3 monolithic tandem photocell structure","authors":"Pierre Gérard Darel Kond Ngue , Ariel Teyou Ngoupo , Aimé Magloire Ntouga Abena , Hichem Bencherif , Ismail Hossain , Jean-Marie Bienvenu Ndjaka","doi":"10.1016/j.micrna.2024.208057","DOIUrl":null,"url":null,"abstract":"<div><div>This paper focuses on the numerical modeling of the quaternary alloy Cd<sub><em>x</em></sub>Sb<sub>2-<em>x</em></sub>(S<sub>1-<em>y</em></sub>Se<sub><em>y</em></sub>)<sub>3</sub> as a lower cell absorber in an Sb<sub>2</sub>S<sub>3</sub>-based tandem system. To this end, the governing laws of the evolution of the band gap and the electron affinity of the alloy are established and solved with reference to the defined substitution proportions. The results show that the band gap of the alloy decreases from 1.88 eV to 0.93 eV with increasing <em>x</em> and <em>y</em> proportions. In a planar heterojunction of FTO/(ZnO/TiO<sub>2</sub>)/Absorber/Spiro-OMeTAD/Au configuration, the Cd<sub><em>x</em></sub>Sb<sub>2-<em>x</em></sub>(S<sub>1-<em>y</em></sub>Se<sub><em>y</em></sub>)<sub>3</sub> alloy, used as the absorber, exhibits a maximum efficiency of 8.81 %, which surpasses the 5.08 % efficiency of the Sb<sub>2</sub>S<sub>3</sub> absorber. For specific band parameters and proportions (Eg = 1.22 eV, χ = 4.25 eV, <em>x</em> = 0.04 and <em>y</em> = 0.9), Cd<sub>0.04</sub>Sb<sub>1.96</sub>(S<sub>0.1</sub>Se<sub>0.9</sub>)<sub>3</sub> is used as the lower solar cell absorber in a tandem structure based on Sb<sub>2</sub>S<sub>3</sub> as the upper cell. After optimization of the absorber thickness, the upper and lower cells demonstrated an efficiency of 8.42 % and 13.74 %. A preliminary simulation of the Sb<sub>2</sub>S<sub>3</sub>/Cd<sub>0.04</sub>Sb<sub>1.96</sub>(S<sub>0.1</sub>Se<sub>0.9</sub>)<sub>3</sub> tandem structure indicated an efficiency of 17.98 %. Following the matching of the current between the upper and lower cells for a thickness of 0.4 μm of each absorber, the Sb<sub>2</sub>S<sub>3</sub>/Cd<sub>0.04</sub>Sb<sub>1.96</sub>(S<sub>0.1</sub>Se<sub>0.9</sub>)<sub>3</sub> tandem solar cell demonstrated an efficiency of 16.19 %. This difference in performance is explained by the lower cell operating in saturation. These results illustrate the prospective applicability of Cd<sub><em>x</em></sub>Sb<sub>2-<em>x</em></sub>(S<sub>1-<em>y</em></sub>Se<sub><em>y</em></sub>)<sub>3</sub> as an absorber material in both single and multi-junction solar cells.</div></div>","PeriodicalId":100923,"journal":{"name":"Micro and Nanostructures","volume":"198 ","pages":"Article 208057"},"PeriodicalIF":2.7000,"publicationDate":"2025-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Micro and Nanostructures","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S2773012324003078","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, CONDENSED MATTER","Score":null,"Total":0}
引用次数: 0
Abstract
This paper focuses on the numerical modeling of the quaternary alloy CdxSb2-x(S1-ySey)3 as a lower cell absorber in an Sb2S3-based tandem system. To this end, the governing laws of the evolution of the band gap and the electron affinity of the alloy are established and solved with reference to the defined substitution proportions. The results show that the band gap of the alloy decreases from 1.88 eV to 0.93 eV with increasing x and y proportions. In a planar heterojunction of FTO/(ZnO/TiO2)/Absorber/Spiro-OMeTAD/Au configuration, the CdxSb2-x(S1-ySey)3 alloy, used as the absorber, exhibits a maximum efficiency of 8.81 %, which surpasses the 5.08 % efficiency of the Sb2S3 absorber. For specific band parameters and proportions (Eg = 1.22 eV, χ = 4.25 eV, x = 0.04 and y = 0.9), Cd0.04Sb1.96(S0.1Se0.9)3 is used as the lower solar cell absorber in a tandem structure based on Sb2S3 as the upper cell. After optimization of the absorber thickness, the upper and lower cells demonstrated an efficiency of 8.42 % and 13.74 %. A preliminary simulation of the Sb2S3/Cd0.04Sb1.96(S0.1Se0.9)3 tandem structure indicated an efficiency of 17.98 %. Following the matching of the current between the upper and lower cells for a thickness of 0.4 μm of each absorber, the Sb2S3/Cd0.04Sb1.96(S0.1Se0.9)3 tandem solar cell demonstrated an efficiency of 16.19 %. This difference in performance is explained by the lower cell operating in saturation. These results illustrate the prospective applicability of CdxSb2-x(S1-ySey)3 as an absorber material in both single and multi-junction solar cells.