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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Collin, Stéphane
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (21/21 displayed)
- 2024Quantitative assessment of selenium diffusion and passivation in CdSeTe solar cells probed by spatially resolved cathodoluminescencecitations
- 2023Humidity‐Induced Degradation Processes of Halide Perovskites Unveiled by Correlative Analytical Electron Microscopycitations
- 2021Imaging CdCl 2 defect passivation and formation in polycrystalline CdTe films by cathodoluminescencecitations
- 2020Erbium-doped oxide for optical gain on hybrid silicon photonics platforms (Student Paper)
- 2020Backside light management of 4-terminal bifacial perovskite/silicon tandem PV modules evaluated under realistic conditionscitations
- 2019Development of reflective back contacts for high-efficiency ultrathin Cu(In,Ga)Se2 solar cellscitations
- 2017Coupling Optical and Electrical Modelling for the study of a-Si:H-based nanowire Array Solar Cellscitations
- 2017Coupling Optical and Electrical Modelling for the study of a-Si:H-based nanowire Array Solar Cellscitations
- 2017Cathodoluminescence mapping for the determination of n-type doping in single GaAs nanowires
- 2017Cathodoluminescence mapping for the determination of n-type doping in single GaAs nanowires
- 2017Interface dipole and band bending in the hybrid p − n heterojunction Mo S 2 / GaN ( 0001 )citations
- 2017Interface dipole and band bending in the hybrid p − n heterojunction Mo S 2 / GaN ( 0001 )citations
- 2016Ultrathin Epitaxial Silicon Solar Cells with Inverted Nanopyramid Arrays for Efficient Light Trappingcitations
- 2015Ultrathin nanostructured c-Si solar cells by low temperature and scalable processes
- 2013Multi-resonant absorption in ultra-thin silicon solar cells with metallic nanowirescitations
- 2013Multi-resonant absorption in ultra-thin silicon solar cells with metallic nanowirescitations
- 2013Metal–dielectric bi-atomic structure for angular-tolerant spectral filteringcitations
- 20123D modeling of metamaterials at oblique incidence and effective analysis
- 20123D modeling of metamaterials at oblique incidence and effective analysis
- 2012Nanopatterned front contact for broadband absorption in ultra-thin amorphous silicon solar cellscitations
- 2012Nanopatterned front contact for broadband absorption in ultra-thin amorphous silicon solar cellscitations
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article
Coupling Optical and Electrical Modelling for the study of a-Si:H-based nanowire Array Solar Cells
Abstract
Coupled optical/electrical simulations have been performed on solar cells consisting in arrays of p‐i‐n radial nanowires based on crystalline p‐type silicon (c‐Si) core/hydrogenated amorphous silicon (a‐Si:H) shell heterojunctions. Three‐dimensional (3D) optical calculations based on rigorous coupled wave analysis (RCWA) are firstly performed and then coupled to a semiconductor device simulator that exploits the radial symmetry of the nanowires. By varying either the doping concentration of the c‐Si core, or the work function of the Al‐doped ZnO (AZO) back contact we can separate and originally highlight the contribution to the cells performance of the nanowires themselves (the radial cell) from the planar part in between the nanowires (the planar cell). We show that the short‐circuit current density (Jsc) only depends on the doping of the c‐Si core indicating that it is mainly influenced by the radial cell. On the contrary the open‐circuit voltage (Voc) is strongly affected by the back contact conditions (AZO work function), revealing an important impact of the interspacing between the nanowires on the characteristics of the entire nanowire array. We explain this strong influence of the back contact conditions by the fact that it determines the band‐bending in the a‐Si:H absorber shell touching the AZO, i.e. in the planar part. Therefore, it directly impacts the potential drop (Vbi) in the same area. For low AZO work functions, the dark current density (Jdark) is increased in the planar region, where Vbi is lower, which degrades the Voc of the entire cell.