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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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Rostohar, Danijela
Coventry University
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (7/7 displayed)
- 2024The Effect of Laser Shock Peening (LSP) on the Surface Roughness and Fatigue Behavior of Additively Manufactured Ti-6Al-4V Alloycitations
- 2023Surface integrity of SLM manufactured meso-size gears in laser shock peening without coatingcitations
- 2022Improvements of metal additive manufactured AISI 304L and Ti6Al4V parts by using laser shock peening as a post-process techniquecitations
- 2020Fabrication of functional superhydrophobic surfaces on carbon fibre reinforced plastics by IR and UV direct laser interference patterningcitations
- 2020Micromachining of Invar with 784 Beams Using 1.3 ps Laser Source at 515 nmcitations
- 2019Non-fluorinated superhydrophobic Al7075 aerospace alloy by ps laser processingcitations
- 2016Part 2citations
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article
Part 2
Abstract
<p>We investigate selective patterning of ultra-thin 20 nm Indium Tin Oxide (ITO) thin films on glass substrates, using 343, 515, and 1030 nm femtosecond (fs), and 1030 nm picoseconds (ps) laser pulses. An ablative removal mechanism is observed for all wavelengths at both femtosecond and picoseconds time-scales. The absorbed threshold fluence values were determined to be 12.5 mJ cm<sup>-</sup><sup>2</sup> at 343 nm, 9.68 mJ cm<sup>-</sup><sup>2</sup> at 515 nm, and 7.50 mJ cm<sup>-</sup><sup>2</sup> at 1030 nm for femtosecond and 9.14 mJ cm<sup>-</sup><sup>2</sup> at 1030 nm for picosecond laser exposure. Surface analysis of ablated craters using atomic force microscopy confirms that the selective removal of the film from the glass substrate is dependent on the applied fluence. Film removal is shown to be primarily through ultrafast lattice deformation generated by an electron blast force. The laser absorption and heating process was simulated using a two temperature model (TTM). The predicted surface temperatures confirm that film removal below 1 J cm<sup>-2</sup> to be predominately by a non-thermal mechanism.</p>