| People | Locations | Statistics |
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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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Nayan, Nafarizal
Laboratoire Bourguignon des Matériaux et Procédés
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (24/24 displayed)
- 2023Analysis of the Anticorrosion Performance and Antibacterial Efficacy of Ti-Based Ceramic Coatings for Biomedical Applicationscitations
- 2021Synthesis, characterization and biophysical evaluation of the 2D Ti2CTx MXene using 3D spheroid-type culturescitations
- 2019Effects of Laser Radiation on the Optical and Electrical Properties of ITO Thin Films Deposited by RF Sputteringcitations
- 2019Photochemical reduction of carbonyl group of polyimide by 450 nm diode laser
- 2018Reduced graphene oxide-multiwalled carbon nanotubes hybrid film with low Pt loading as counter electrode for improved photovoltaic performance of dye-sensitised solar cellscitations
- 2018Difference in structural and chemical properties of sol–gel spin coated Al doped TiO2, Y doped TiO2 and Gd doped TiO2 based on trivalent dopantscitations
- 2017The influence of N2 flow rate on Ar and Ti Emission in high-pressure magnetron sputtering system plasmacitations
- 2016Sputter Deposition of Cuprous and Cupric Oxide Thin Films Monitored by Optical Emission Spectroscopy for Gas Sensing Applicationscitations
- 2016Correlation between Microstructure of Copper Oxide Thin Films and its Gas Sensing Performance at Room Temperaturecitations
- 2015Spectroscopic Studies of Magnetron Sputtering Plasma Discharge in Cu/O2/Ar Mixture for Copper Oxide Thin Film Fabricationcitations
- 2015Fabrication of inverted bulk heterojunction organic solar cells based on conjugated P3HT:PCBM using various thicknesses of ZnO buffer layercitations
- 2015Influence of TiO2 thin film annealing temperature on electrical properties synthesized by CVD technique
- 2014Glass etching for cost-effective microchannels fabricationcitations
- 2014Physical and optical studies on ZnO films by SOL-GELcitations
- 2014Fabrication and Characterisation of the Electrical and Physical Properties of the Mask Printed Graphite Paste Electrodes on Paper Substratescitations
- 2013Oxide semiconductors for solar to chemical energy conversion: nanotechnology approachcitations
- 2013Biophysical characteristics of cells cultured on cholesteryl ester liquid crystals.citations
- 2013Morphology, topography and thickness of copper oxide thin films deposited using magnetron sputtering techniquecitations
- 2012Characterization of TiAlBN nanocomposite coating deposited via radio frequency magnetron sputtering using single hot-pressed targetcitations
- 2012Plasma properties of RF magnetron sputtering system using Zn targetcitations
- 2012Sol-gel Synthesis of TiO 2 Thin Films from In-house Nano-TiO 2 Powder
- 2012Corrosion Behavior of AZ91 Mg-Alloy Coated with AlN and TiN in NaCl and Hank's Solutioncitations
- 2010Structural and Electrical Properties of TiO2 Thin Film Derived from Sol-gel Method using Titanium (IV) Butoxide
- 2010Optimization of RF magnetron sputtering plasma using Zn targetcitations
Places of action
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document
Morphology, topography and thickness of copper oxide thin films deposited using magnetron sputtering technique
Abstract
Cupric Oxide (CuO) is one of the p-type metal oxide semiconductors that are suitable for use in gas sensing device. The copper oxide thin film was prepared on silicon wafer by sputtering of pure copper target at difference deposition time of 5 min, 10 min and 15 min using RF magnetron sputtering technique. Argon flow rate, oxygen flow rate, RF power and working pressure were fixed at 50 sccm, 8 sccm, 400 W and 22.5 mTorr, respectively. The influence of the deposition time towards the surface morphology, topography and thickness has been investigated. SEM and AFM analysis showed that the grain size of the films increases with the increase of deposition time. However, the surface structure of the films remains the same. In addition, it is noticed that when the deposition time increased, the surface of the films becomes rougher. The deposition rate was approximately 29 nm/min, and it was evaluated from the film thickness deposited at several times.