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Study of a Lead-Free Perovskite Solar Cell Using CZTS as HTL to Achieve a 20% PCE by SCAPS-1D Simulation

In this paper, a n-i-p planar heterojunction simulation of Sn-based iodide perovskite solar cell (PSC) is proposed. The solar cell structure consists of a Fluorine-doped tin oxide (FTO) substrate on which titanium oxide (TiO(2)) is placed; this material will act as an electron transporting layer (ET...

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Detalles Bibliográficos
Autores principales: Piñón Reyes, Ana C., Ambrosio Lázaro, Roberto C., Monfil Leyva, Karim, Luna López, José A., Flores Méndez, Javier, Heredia Jiménez, Aurelio H., Muñoz Zurita, Ana L., Severiano Carrillo, Francisco, Ojeda Durán, Esteban
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8707567/
https://www.ncbi.nlm.nih.gov/pubmed/34945358
http://dx.doi.org/10.3390/mi12121508
Descripción
Sumario:In this paper, a n-i-p planar heterojunction simulation of Sn-based iodide perovskite solar cell (PSC) is proposed. The solar cell structure consists of a Fluorine-doped tin oxide (FTO) substrate on which titanium oxide (TiO(2)) is placed; this material will act as an electron transporting layer (ETL); then, we have the tin perovskite CH(3)NH(3)SnI(3) (MASnI(3)) which is the absorber layer and next a copper zinc and tin sulfide (CZTS) that will have the function of a hole transporting layer (HTL). This material is used due to its simple synthesis process and band tuning, in addition to presenting good electrical properties and stability; it is also a low-cost and non-toxic inorganic material. Finally, gold (Au) is placed as a back contact. The lead-free perovskite solar cell was simulated using a Solar Cell Capacitance Simulator (SCAPS-1D). The simulations were performed under AM 1.5G light illumination and focused on getting the best efficiency of the solar cell proposed. The thickness of MASnI(3) and CZTS, band gap of CZTS, operating temperature in the range between 250 K and 350 K, acceptor concentration and defect density of absorber layer were the parameters optimized in the solar cell device. The simulation results indicate that absorber thicknesses of 500 nm and 300 nm for CZTS are appropriate for the solar cell. Further, when optimum values of the acceptor density (N(A)) and defect density (N(t)), 10(16) cm(−3) and 10(14) cm(−3), respectively, were used, the best electrical values were obtained: J(sc) of 31.66 mA/cm(2), V(oc) of 0.96 V, FF of 67% and PCE of 20.28%. Due to the enhanced performance parameters, the structure of the device could be used in applications for a solar energy harvesting system.