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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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Döbeli, Max
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (31/31 displayed)
- 2024Electrosynthesis-Induced Pt Skin Effect in Mesoporous Ni-Rich Ni-Pt Thin Films for Hydrogen Evolution Reaction
- 2023Momentum-resolved electronic structure of LaTiO2N photocatalysts by resonant Soft-X-ray ARPEScitations
- 2022Mechanical properties of atomic-layer-deposited Al 2 O 3 /Y 2 O 3 nanolaminate films on aluminum toward protective coatingscitations
- 2022Unravelling the Origin of Ultra‐Low Conductivity in SrTiO$_3$ Thin Films: Sr Vacancies and Ti on A‐Sites Cause Fermi Level Pinningcitations
- 2021Ferromagnetic insulating epitaxially strained La$_2$NiMnO$_6$ thin films grown by sputter depositioncitations
- 2020A combinatorial guide to phase formation and surface passivation of tungsten titanium oxide prepared by thermal oxidationcitations
- 2020Monolithic thin-film chalcogenide–silicon tandem solar cells enabled by a diffusion barriercitations
- 2020Electroless deposition of Ni–Fe alloys on scaffolds for 3D nanomagnetismcitations
- 2020Persistent Double-Layer Formation in Kesterite Solar Cells: A Critical Reviewcitations
- 2020Persistent Double-Layer Formation in Kesterite Solar Cells: A Critical Reviewcitations
- 2020Thickness-dependent microstructural properties of heteroepitaxial (00.1) CuFeO2 thin films on (00.1) sapphire by pulsed laser depositioncitations
- 2020Lithium garnet Li 7 La 3 Zr 2 O 12 electrolyte for all-solid-state batteries: closing the gap between bulk and thin film Li-ion conductivitiescitations
- 2020The curious mechanism of irradiation-induced cryogenic grain growth in tungsten thin films: a pathway to single crystalscitations
- 2019Anodizing of Self-Passivating WxTi1–x Precursors for WxTi1–xOn Oxide Alloys with Tailored Stabilitycitations
- 2019Anodizing of self-passivating W x Ti 1– x precursors for W x Ti 1– x O n oxide alloys with tailored stabilitycitations
- 2018Amorphous gallium oxide grown by low-temperature PECVDcitations
- 2018Substrate purity effect on the defect formation and properties of amorphous anodic barrier Al 2 O 3citations
- 2018Epitaxial thin films as a model system for Li-Ion conductivity in Li 4 Ti 5 O 12citations
- 2018Mechanical Properties of Advanced Gas-Cooled Reactor Stainless Steel Cladding After Irradiationcitations
- 2018Investigation of the foil structure and corrosion mechanisms of modern Zwischgold using advanced analysis techniquescitations
- 2017Stoichiometric control of the density of states in PbS colloidal quantum dot solidscitations
- 2017Reaction and growth mechanisms in Al 2 O 3 deposited via atomic layer deposition: elucidating the hydrogen sourcecitations
- 2017Versatile two-dimensional transition metal dichalcogenides
- 2016TiN-buffered substrates for photoelectrochemical measurements of oxynitride thin filmscitations
- 2016The importance of pressure and mass ratios when depositing multi-element oxide thin films by pulsed laser depositioncitations
- 2015Hydrogenated indium oxide window layers for high-efficiency Cu(In,Ga)Se 2 solar cellscitations
- 2014Laser deposition and direct-writing of thermoelectric misfit cobaltite thin filmscitations
- 2013SIMS of thin films grown by pulsed laser deposition on isotopically labeled substratescitations
- 2012Lanthanum nickelate thin films deposited by spray pyrolysis: Crystallization, microstructure and electrochemical propertiescitations
- 2011Crystallization and grain growth characteristics of yttria-stabilized zirconia thin films grown by pulsed laser depositioncitations
- 2009Optical properties of nitrogen-substituted strontium titanate thin films prepared by pulsed laser depositioncitations
Places of action
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conferencepaper
Versatile two-dimensional transition metal dichalcogenides
Abstract
Two-dimensional transition metal dichalcogenides (2D-TMDCs), such as MoS2, have emerged as a<br/>new class of semiconducting materials with distinct optical and electrical properties. The availability<br/>of 2D-TMDCs with distinct band gaps allows for unlimited combinations of TMDC monolayers<br/>(MLs) and enables engineering of van der Waals (vdW) heterostructures with characteristics<br/>fundamentally different compared to the conventional 3D-covalently bounded heterostructures.<br/>Although various 2D materials have been successfully synthesized by mechanical exfoliation or<br/>chemical vapor deposition (CVD), a strategy for the fabrication of 2D heterostructures must be<br/>developed. Here we demonstrate a novel approach for the bottom-up synthesis of TMDC monolayers, namely Pulsed Laser Deposition (PLD) combined with a sulfur evaporation beam. PLD relies on the use of a pulsed laser (ns pulse duration) to induce material transfer from a solid source (such as a sintered target of MoS2) to a substrate (such as Si or sapphire). The deposition rate in PLD is typically much less than a monolayer per pulse, meaning that the number of MLs can be controlled by a careful selection of the number of laser pulses. In the paper, we will discuss the growth of high-quality MoS2 in the form of one or several MLs over large areas and several substrates, such as sapphire, SiO2/Si and indium tin oxide (ITO). This approach allows the synthesis of 2D-TMDCs without the use of catalyst and with a good control of the sulfur vacancies. We have found that the absorption spectra of the MoS2 films exhibit distinct excitonic peaks at ~1.8 and ~2 eV when grown in the presence of a sulfur evaporation beam as compared to those deposited in vacuum. The structure of the PLD-grown MoS2 films will be further discussed based Raman spectroscopy analysis, photoluminescence, as composition/thickness determined by Rutherford backscattering (RBS). Some challenging issues and future directions on the use of PLD for the synthesis of complex heterostructures by PLD will be discussed.