People | Locations | Statistics |
---|---|---|
Naji, M. |
| |
Motta, Antonella |
| |
Aletan, Dirar |
| |
Mohamed, Tarek |
| |
Ertürk, Emre |
| |
Taccardi, Nicola |
| |
Kononenko, Denys |
| |
Petrov, R. H. | Madrid |
|
Alshaaer, Mazen | Brussels |
|
Bih, L. |
| |
Casati, R. |
| |
Muller, Hermance |
| |
Kočí, Jan | Prague |
|
Šuljagić, Marija |
| |
Kalteremidou, Kalliopi-Artemi | Brussels |
|
Azam, Siraj |
| |
Ospanova, Alyiya |
| |
Blanpain, Bart |
| |
Ali, M. A. |
| |
Popa, V. |
| |
Rančić, M. |
| |
Ollier, Nadège |
| |
Azevedo, Nuno Monteiro |
| |
Landes, Michael |
| |
Rignanese, Gian-Marco |
|
Maguire, Paul
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (22/22 displayed)
- 2023A Single‐Step Process to Produce Carbon Nanotube‐Zinc Compound Hybrid Materialscitations
- 2021Carrier extraction from metallic perovskite oxide nanoparticlescitations
- 2021Understanding plasma–ethanol non-equilibrium electrochemistry during the synthesis of metal oxide quantum dotscitations
- 2020The analysis of dissolved inorganic carbon in liquid using a microfluidic conductivity sensor with membrane separation of CO2citations
- 2019Nanostructured perovskite solar cells
- 2018Zero-dimensional methylammonium iodo bismuthate solar cells and synergistic interactions with silicon nanocrystalscitations
- 2018Microplasma-assisted electrochemical synthesis of Co3O4 nanoparticles in absolute ethanol for energy applicationscitations
- 2017Zero-dimensional methylammonium iodo bismuthate solar cells and synergistic interactions with silicon nanocrystalscitations
- 2017Charge carrier localised in zero-dimensional (CH 3 NH 3 ) 3 Bi 2 1 9 clusterscitations
- 2017Charge carrier localised in zero-dimensional (CH3NH3)3Bi219 clusterscitations
- 2017Charge carrier localised in zero-dimensional (CH3NH3)3Bi219 clusterscitations
- 2017Charge carrier localised in zero-dimensional (CH3NH3)3Bi2I9 clusterscitations
- 2011Structural and surface energy analysis of nitrogenated ta-C filmscitations
- 2009Electrical and Raman spectroscopic studies of vertically aligned multi-walled carbon nanotubes.citations
- 2009Substrate effects on the microstructure of hydrogenated amorphous carbon filmscitations
- 2007Intrinsic mechanical properties of ultra-thin amorphous carbon layerscitations
- 2006Measuring the thickness of ultra-thin diamond-like carbon filmscitations
- 2004Platelet adhesion on silicon modified hydrogenated amorphous carbon films.citations
- 2001Electrical characteristics of nitrogen incorporated hydrogenated amorphous carboncitations
- 2001Intrinsic stress measured on ultra-thin amorphous carbon films deposited on AFM cantileverscitations
- 2001The insulating properties of a-C:H on silicon and metal substratescitations
- 2000Nitrogen doping of amorphous DLC films by rf plasma dissociated nitrogen atom surface bombardment in a vacuumcitations
Places of action
Organizations | Location | People |
---|
article
Intrinsic mechanical properties of ultra-thin amorphous carbon layers
Abstract
n this work, we extracted the film's hardness ( H F ) of ultra-thin diamond-like carbon layers by simultaneously taking into account the tip blunting and the substrate effect. As compared to previous approaches, which did not consider tip blunting, this resulted in marked differences (30–100%) for the H F value of the thinner carbon coatings. We find that the nature of the substrate influences this intrinsic film parameter and hence the growth mechanisms. Moreover, the H F values generally increase with film thickness. The 10 nm and 50 nm thick hydrogenated amorphous carbon (a-C:H) films deposited onto Si have H F values of, respectively, ∼26 GPa and ∼31 GPa whereas the 10 nm and 50 nm thick tetrahedral amorphous carbon (t-aC) films deposited onto Si have H F values of, respectively, ∼29 GPa and ∼38 GPa. Both the a-C:H and t-aC materials also show higher density and refractive index values for the thicker coatings, as measured, respectively by X-ray reflectometry and optical profilometry analysis. However, the Raman analysis of the a-C:H samples show bonding characteristics which are independent of the film thickness. This indicates that in these ultra-thin hydrogenated carbon films, the arrangement of sp 2 clusters does not relate directly to the hardness of the film.