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. 2021 Mar 30;11:7179. doi: 10.1038/s41598-021-86738-6

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© The Author(s) 2021

Open AccessThis article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/.

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(a) Variation of the short-circuit current, $J_{SC}$ , for the optimum design (filled circles) and the unmodified planar cell (open circles) as a function of the thickness of the active layer, $t_{i - aSi : H}$ . (b) Short-circuit current as a function of the angle of incidence for the optimum design of the cell plus the nano-dimer (filled circles), and the planar solar cell (open circles).