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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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Orava, Jiri
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (8/8 displayed)
- 2024Tailoring microstructure and properties of CuZrAl(Nb) metallic-glass–crystal composites and nanocrystalline alloys obtained by flash-annealingcitations
- 2022Phase-formation maps of CuZrAlCo metallic glass explored by in situ ultrafast techniquescitations
- 2021In situ correlation between metastable phase-transformation mechanism and kinetics in a metallic glass.
- 2021In situ correlation between metastable phase-transformation mechanism and kinetics in a metallic glasscitations
- 2021In situ correlation between metastable phase-transformation mechanism and kinetics in a metallic glass
- 2021In situ correlation between metastable phase-transformation mechanism and kinetics in a metallic glass
- 2020Fast-current-heating devices to study in situ phase formation in metallic glasses by using high-energy synchrotron radiationcitations
- 2017In-situ study of athermal reversible photocrystallization in a chalcogenide glasscitations
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article
In-situ study of athermal reversible photocrystallization in a chalcogenide glass
Abstract
<jats:p>The time-resolved Raman measurements reveal a three-stage mechanism of the photostructural changes in Ge25.0Ga9.5Sb0.5S65.0 (containing 0.5 at. % of Er3+) glass under continuous-above-bandgap illumination. These changes are reversible and effectively athermal, in that the local temperature rises to about 60% of the glass-transition temperature and the phase transitions take place in the glass/crystal and not in an equilibrium liquid. In the early stages of illumination, the glassy-network dimensionality changes from a predominantly 3-D to a mixture of 2-D/1-D represented by an increase in the fraction of edge-sharing tetrahedra and the emergence of homonuclear (semi)metallic bonds. This incubation period of the structural rearrangements, weakly thermally activated with an energy of ∼0.16 eV, facilitates a reversible photocrystallization. The photocrystallization rate in the glass is comparable to that achieved by thermal crystallization from supercooled liquid at large supercooling. Almost complete re-amorphization can be achieved in about an hour by reducing the incident laser-power density by a factor of ten. Glass-ceramic composites—with varying glass-to-crystal fraction—can be obtained by ceasing the illumination during re-amorphization. Microstructural imaging reveals photoinduced mass transport and the formation of columnar-porous structures. This shows the potential for a bond-specific engineering of glassy structures for photonic applications with a spatial resolution unachievable by thermal annealing.</jats:p>