693.932 PEOPLE
| 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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Jacobsen, Karsten Wedel
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (30/30 displayed)
- 2020Minimum-strain symmetrization of Bravais latticescitations
- 2019High-Entropy Alloys as a Discovery Platform for Electrocatalysiscitations
- 2019Shining Light on Sulfide Perovskites: LaYS 3 Material Properties and Solar Cellscitations
- 2019Shining Light on Sulfide Perovskites: LaYS3 Material Properties and Solar Cellscitations
- 2018Machine learning-based screening of complex molecules for polymer solar cellscitations
- 2018Computational Screening of Light-absorbing Materials for Photoelectrochemical Water Splittingcitations
- 2017Sulfide perovskites for solar energy conversion applications: computational screening and synthesis of the selected compound LaYS 3citations
- 2017Nanocrystalline metals: Roughness in flatlandcitations
- 2017Determination of low-strain interfaces via geometric matchingcitations
- 2017Sulfide perovskites for solar energy conversion applications: computational screening and synthesis of the selected compound LaYS3citations
- 2016Atomically Thin Ordered Alloys of Transition Metal Dichalcogenides: Stability and Band Structurescitations
- 2016Defect-Tolerant Monolayer Transition Metal Dichalcogenidescitations
- 2015Band-gap engineering of functional perovskites through quantum confinement and tunnelingcitations
- 2013Bandgap Engineering of Double Perovskites for One- and Two-photon Water Splittingcitations
- 2013Stability and bandgaps of layered perovskites for one- and two-photon water splittingcitations
- 2013Density functional theory studies of transition metal nanoparticles in catalysis
- 2012Conventional and acoustic surface plasmons on noble metal surfaces: a time-dependent density functional theory studycitations
- 2012Computational screening of perovskite metal oxides for optimal solar light capturecitations
- 2012Spatially resolved quantum plasmon modes in metallic nano-films from first-principles
- 2011Nonlocal Screening of Plasmons in Graphene by Semiconducting and Metallic Substrates:First-Principles Calculationscitations
- 2011Nonlocal Screening of Plasmons in Graphene by Semiconducting and Metallic Substratescitations
- 2011Trends in Metal Oxide Stability for Nanorods, Nanotubes, and Surfacescitations
- 2010Computer simulations of nanoindentation in Mg-Cu and Cu-Zr metallic glassescitations
- 2010Computer simulations of nanoindentation in Mg-Cu and Cu-Zr metallic glassescitations
- 2010Graphene on metals: A van der Waals density functional studycitations
- 2006Atomistic simulation study of the shear-band deformation mechanism in Mg-Cu metallic glassescitations
- 2004Simulation of Cu-Mg metallic glass: Thermodynamics and structurecitations
- 2004Atomistic simulations of Mg-Cu metallic glasses: Mechanical propertiescitations
- 2004Simulations of intergranular fracture in nanocrystalline molybdenumcitations
- 2003A maximum in the strength of nanocrystalline copper
Places of action
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article
Graphene on metals: A van der Waals density functional study
Abstract
We use density functional theory (DFT) with a recently developed van der Waals density functional (vdW-DF) to study the adsorption of graphene on Co, Ni, Pd, Ag, Au, Cu, Pt, and Al(111) surfaces. In contrast to the local-density approximation (LDA) which predicts relatively strong binding for Ni,Co, and Pd, the vdW-DF predicts weak binding for all metals and metal-graphene distances in the range 3.40–3.72 Å. At these distances the graphene band structure as calculated with DFT and the many-body G0W0 method is basically unaffected by the substrate, in particular there is no opening of a band gap at the K point.