2024
DOI: 10.1002/adom.202302121
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3D Radial Junctions for Robust and Flexible Optoelectronics

Shaobo Zhang,
Linwei Yu

Abstract: Marrying nanostructures with thin films is a recent trend in flexible optoelectronics to improve light trapping and mechanical stability. Radial junction (RJ) a‐Si:H thin film optoelectronics, directly deposited upon the vapor‐liquid‐solid (VLS) grown silicon nanowires (SiNWs), can pave the way to achieving excellent flexibility and a high power‐to‐weight ratio (PTWR). Thanks to their vertical‐standing geometry, SiNWs framework can enhance the mechanical stability of RJ units, by keeping the working region far… Show more

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Cited by 2 publications
(1 citation statement)
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“…Nowadays, crystalline silicon (c-Si) based solar cells dominate ∼95% of the photovoltaic (PV) market . So, even an insignificant performance improvement of these commercial c-Si solar cells, to seek a more competitive levelized cost of electricity (LCOE), is highly valuable. Until now, a bunch of strategies have been demonstrated, such as constructing different stacked tandem even multijunction cell architecture (perovskite/c-Si tandem, polymer/perovskite tandem, or amorphous Si/c-Si tandem, and so on), to overcome the Shockley-Queisser limit of ∼33% for single-junction c-Si solar cells . For example, the perovskite thin film materials, attractive in recent years for their high spectral response, and low cost as well as a high initial performance of a single junction, can be used as the top cell, to form perovskite/Si tandem solar cells. , However, there are lots of challenges in designing/fabricating tandem/multijunction, such as photocurrent matching, tunnel junction, and so on. , Besides, the high-energy photons, particularly in the ultraviolet (UV) wavelength region, which have energy much higher than the bandgap, are mostly absorbed nearly at the surface of Si devices but provide few effective carriers for device performance because of more defect states at the interface .…”
mentioning
confidence: 99%
“…Nowadays, crystalline silicon (c-Si) based solar cells dominate ∼95% of the photovoltaic (PV) market . So, even an insignificant performance improvement of these commercial c-Si solar cells, to seek a more competitive levelized cost of electricity (LCOE), is highly valuable. Until now, a bunch of strategies have been demonstrated, such as constructing different stacked tandem even multijunction cell architecture (perovskite/c-Si tandem, polymer/perovskite tandem, or amorphous Si/c-Si tandem, and so on), to overcome the Shockley-Queisser limit of ∼33% for single-junction c-Si solar cells . For example, the perovskite thin film materials, attractive in recent years for their high spectral response, and low cost as well as a high initial performance of a single junction, can be used as the top cell, to form perovskite/Si tandem solar cells. , However, there are lots of challenges in designing/fabricating tandem/multijunction, such as photocurrent matching, tunnel junction, and so on. , Besides, the high-energy photons, particularly in the ultraviolet (UV) wavelength region, which have energy much higher than the bandgap, are mostly absorbed nearly at the surface of Si devices but provide few effective carriers for device performance because of more defect states at the interface .…”
mentioning
confidence: 99%