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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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Azimi, Zahra
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Publications (5/5 displayed)
- 2022Tuning the crystal structure and optical properties of selective area grown InGaAs nanowirescitations
- 2022Epitaxial Growth of GaAs Nanowires on Synthetic Mica by Metal–Organic Chemical Vapor Depositioncitations
- 2022Effective Passivation of InGaAs Nanowires for Telecommunication Wavelength Optoelectronicscitations
- 2021Tuning the crystal structure and optical properties of selective area grown InGaAs nanowires
- 2021Understanding the role of facets and twin defects in the optical performance of GaAs nanowires for laser applicationscitations
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article
Effective Passivation of InGaAs Nanowires for Telecommunication Wavelength Optoelectronics
Abstract
<p>Catalyst-free InGaAs nanowires are promising building blocks for optoelectronic devices operating at telecommunication wavelengths. Despite progress, the applications of InGaAs nanowires remain limited due to their high density of surface states that degrade their optical properties. Here, InGaAs nanowires with superior optical properties are achieved by effectively suppressing their surface states with an InP passivation shell. Optimal InP shell growth conditions and thickness to maximize the minority carrier lifetime are identified. The photoluminescence intensity of these passivated InGaAs nanowires is up to three orders of magnitude higher than that of their bare counterparts. Moreover, a long minority carrier lifetime of up to ≈13 ns is measured with these passivated nanowires at room temperature. Optimal passivation of InGaAs nanowires with an emission wavelength of 1530 nm results in an ultra-low surface recombination velocity of ≈280 cm s<sup>−1</sup>. In addition to the shell, the crystal structure of these nanowires plays an important role in the luminescence intensity. Combined cathodoluminescence mapping and high-resolution transmission electron microscopy along the nanowires reveal significantly lower emission intensities in wurtzite predominant sections of the nanowires than zinc blende predominant ones.These insights on the optimal passivation of InGaAs provide directions for engineering high-performance nanoscale-devices in the telecommunication wavelength.</p>