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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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Yang, Xinbo
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Publications (5/5 displayed)
- 2017Passivation and carrier selectivity of TiO2 contacts combined with different passivation layers and electrodes for silicon solar cellscitations
- 2015Ion-implanted laser-annealed p+ and n+ Regionscitations
- 2015Passivated contacts to laser doped p+ and n+ regionscitations
- 2014The impact of SiO2/SiNrm x stack thickness on laser doping of silicon solar cellcitations
- 2013Secondary electron microscopy dopant contrast image (SEMDCI) for laser dopingcitations
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article
The impact of SiO2/SiNrm x stack thickness on laser doping of silicon solar cell
Abstract
<p>Laser doping of semiconductors has been the subject of intense research over the past decades. Previous work indicates that the use of SiO <sub>2</sub>/SiN <sub> x</sub> stacks instead of a single dielectric film as the anti-reflection coating and passivation layer results in laser doped lines with superior properties. In this paper, the impact of the SiN<sub> x</sub> layer thickness in the SiO <sub>2</sub>/SiN<sub> x</sub> stacks on the properties of laser doped lines is investigated through resistance measurements of the laser doped line and the silicon-metal contact and the doping profile near the edge of the dielectric window, the latter being an important factor in determining the likelihood of high recombination or even shunting from the subsequent metallization process. Fundamentally, a problem of exposed and undoped silicon near the dielectric window is identified for most of the investigated parameter range. However, optimization of the laser parameters and dielectric film conditions is shown to be capable of preventing or at least minimizing this problem. The results indicate that for the used laser system, samples with thick dielectric stack processed using a low pulse energy and pulse distance yield the most favorable properties, such as low line resistance and low contact resistivity. Under these conditions, the laser doped regions laterally extend underneath the dielectric films, thus reducing the likelihood of high surface recombination.</p>