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Optimization of the Sb(2)S(3) Shell Thickness in ZnO Nanowire-Based Extremely Thin Absorber Solar Cells

Extremely thin absorber (ETA) solar cells made of ZnO/TiO(2)/Sb(2)S(3) core–shell nanowire heterostructures, using P3HT as the hole-transporting material (HTM), are of high interest to surpass solar cell efficiencies of their planar counterpart at lower material cost. However, no dimensional optimiz...

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Detalles Bibliográficos
Autores principales: Hector, Guislain, Eensalu, Jako S., Katerski, Atanas, Roussel, Hervé, Chaix-Pluchery, Odette, Appert, Estelle, Donatini, Fabrice, Acik, Ilona Oja, Kärber, Erki, Consonni, Vincent
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8777826/
https://www.ncbi.nlm.nih.gov/pubmed/35055217
http://dx.doi.org/10.3390/nano12020198
Descripción
Sumario:Extremely thin absorber (ETA) solar cells made of ZnO/TiO(2)/Sb(2)S(3) core–shell nanowire heterostructures, using P3HT as the hole-transporting material (HTM), are of high interest to surpass solar cell efficiencies of their planar counterpart at lower material cost. However, no dimensional optimization has been addressed in detail, as it raises material and technological critical issues. In this study, the thickness of the Sb(2)S(3) shell grown by chemical spray pyrolysis is tuned from a couple of nanometers to several tens of nanometers, while switching from a partially to a fully crystallized shell. The Sb(2)S(3) shell is highly pure, and the unwanted Sb(2)O(3) phase was not formed. The low end of the thickness is limited by challenges in the crystallization of the Sb(2)S(3) shell, as it is amorphous at nanoscale dimensions, resulting in the low optical absorption of visible photons. In contrast, the high end of the thickness is limited by the increased density of defects in the bulk of the Sb(2)S(3) shell, degrading charge carrier dynamics, and by the incomplete immersion of the P3HT in the structure, resulting in the poor hole collection. The best ETA solar cell with a short-circuit current density of 12.1 mA/cm(2), an open-circuit voltage of 502 mV, and a photovoltaic conversion efficiency of 2.83% is obtained for an intermediate thickness of the Sb(2)S(3) shell. These findings highlight that the incorporation of both the absorber shell and HTM in the core–shell heterostructures relies on the spacing between individual nanowires. They further elaborate the intricate nature of the dimensional optimization of an ETA cell, as it requires a fine-balanced holistic approach to correlate all the dimensions of all the components in the heterostructures.