{"title":"Simulation of CZTSSe Solar Cells with a Hole Transport Layer of Sb2(S1‐x,Sex)3","authors":"Jin Wang, Tianyu Lu, Hongtao Li, Xiaodong Feng","doi":"10.1002/adts.202500956","DOIUrl":null,"url":null,"abstract":"In this study, Cu<jats:sub>2</jats:sub>ZnSn(S,Se)<jats:sub>4</jats:sub> (CZTSSe) solar cell with a hole transport layer (HTL) of Sb<jats:sub>2</jats:sub>(S<jats:sub>1‐x</jats:sub>,Se<jats:sub>x</jats:sub>)<jats:sub>3</jats:sub> is simulated by Solar Cell Capacitance Simulator (SCAPS). First, the effect of the Sb<jats:sub>2</jats:sub>(S<jats:sub>1‐x</jats:sub>,Se<jats:sub>x</jats:sub>)<jats:sub>3</jats:sub> bandgap (E<jats:sub>g</jats:sub>) on device performance is analyzed. When E<jats:sub>g</jats:sub> is 1.5 eV, the valence band offset (VBO) between CZTSSe and Sb<jats:sub>2</jats:sub>(S<jats:sub>1‐x</jats:sub>,Se<jats:sub>x</jats:sub>)<jats:sub>3</jats:sub> is −0.003 eV, forming a nearly flat‐band structure that is favorable for hole transport. Subsequently, several key parameters of the device are optimized. The optimal thickness of the absorber layer is 3.5 µm, and the defect density needs to be controlled below 10<jats:sup>13</jats:sup> cm<jats:sup>−3</jats:sup>. The optimum thickness of the Sb<jats:sub>2</jats:sub>(S<jats:sub>1‐x</jats:sub>,Se<jats:sub>x</jats:sub>)<jats:sub>3</jats:sub> layer is 20 nm, and the ideal doping density is 10<jats:sup>17</jats:sup> cm<jats:sup>−3</jats:sup>. The defect densities at the CZTSSe/Sb<jats:sub>2</jats:sub>(S<jats:sub>1‐x</jats:sub>,Se<jats:sub>x</jats:sub>)<jats:sub>3</jats:sub> and CZTSSe/CdS interfaces should be controlled at 10<jats:sup>14</jats:sup> and 10<jats:sup>13</jats:sup> cm<jats:sup>−2</jats:sup> or less, respectively. The work function of the back‐electrode should be no less than 5.1 eV. Finally, CZTSSe solar cell can achieve the best efficiency of 22.07%. The simulation results demonstrate the potential to provide a new device structure for fabricating high performance CZTSSe devices.","PeriodicalId":7219,"journal":{"name":"Advanced Theory and Simulations","volume":"11 1","pages":""},"PeriodicalIF":2.9000,"publicationDate":"2025-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advanced Theory and Simulations","FirstCategoryId":"5","ListUrlMain":"https://doi.org/10.1002/adts.202500956","RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"MULTIDISCIPLINARY SCIENCES","Score":null,"Total":0}
引用次数: 0
Abstract
In this study, Cu2ZnSn(S,Se)4 (CZTSSe) solar cell with a hole transport layer (HTL) of Sb2(S1‐x,Sex)3 is simulated by Solar Cell Capacitance Simulator (SCAPS). First, the effect of the Sb2(S1‐x,Sex)3 bandgap (Eg) on device performance is analyzed. When Eg is 1.5 eV, the valence band offset (VBO) between CZTSSe and Sb2(S1‐x,Sex)3 is −0.003 eV, forming a nearly flat‐band structure that is favorable for hole transport. Subsequently, several key parameters of the device are optimized. The optimal thickness of the absorber layer is 3.5 µm, and the defect density needs to be controlled below 1013 cm−3. The optimum thickness of the Sb2(S1‐x,Sex)3 layer is 20 nm, and the ideal doping density is 1017 cm−3. The defect densities at the CZTSSe/Sb2(S1‐x,Sex)3 and CZTSSe/CdS interfaces should be controlled at 1014 and 1013 cm−2 or less, respectively. The work function of the back‐electrode should be no less than 5.1 eV. Finally, CZTSSe solar cell can achieve the best efficiency of 22.07%. The simulation results demonstrate the potential to provide a new device structure for fabricating high performance CZTSSe devices.
期刊介绍:
Advanced Theory and Simulations is an interdisciplinary, international, English-language journal that publishes high-quality scientific results focusing on the development and application of theoretical methods, modeling and simulation approaches in all natural science and medicine areas, including:
materials, chemistry, condensed matter physics
engineering, energy
life science, biology, medicine
atmospheric/environmental science, climate science
planetary science, astronomy, cosmology
method development, numerical methods, statistics