| 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 |
|
Marty, Alain
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (23/23 displayed)
- 2024Light-driven Electrodynamics and Demagnetization in Fe$_n$GeTe$_2$ (n = 3, 5) Thin Films
- 2024Atomic‐Layer Controlled Transition from Inverse Rashba–Edelstein Effect to Inverse Spin Hall Effect in 2D PtSe<sub>2</sub> Probed by THz Spintronic Emissioncitations
- 2023Atomic-layer controlled THz Spintronic emission from Epitaxially grown Two dimensional PtSe$_2$/ferromagnet heterostructures
- 2023Nucleation and coalescence of tungsten disulfide layers grown by metalorganic chemical vapor depositioncitations
- 2023Nucleation and coalescence of tungsten disulfide layers grown by metalorganic chemical vapor depositioncitations
- 2022Phonon dynamics and thermal conductivity of PtSe2 thin films: Impact of crystallinity and film thickness on heat dissipation
- 2022Evidence for highly p-type doping and type II band alignment in large scale monolayer WSe2/Se-terminated GaAs heterojunction grown by molecular beam epitaxycitations
- 2021Control of spin-charge conversion in van der Waals heterostructurescitations
- 2021Control of spin–charge conversion in van der Waals heterostructurescitations
- 2019Van der Waals solid phase epitaxy to grow large-area manganese-doped MoSe2 few-layers on SiO2/Sicitations
- 2019Spin-dependent transport characterization in metallic lateral spin valves using one-dimensional and three-dimensional modelingcitations
- 2019Van der Waals solid phase epitaxy to grow large-area manganese-doped MoSe$_2$ few-layers on SiO$_2$/Sicitations
- 2018Impact of a van der Waals interface on intrinsic and extrinsic defects in an MoSe 2 monolayercitations
- 2018Impact of a van der Waals interface on intrinsic and extrinsic defects in an MoSe 2 monolayercitations
- 2018Electrical properties of single crystal Yttrium Iron Garnet ultra-thin films at high temperaturescitations
- 2018Toward efficient spin/charge conversion using topological insulator surface (Conference Presentation)
- 2018Calculation method of spin accumulations and spin signals in nanostructures using spin resistorscitations
- 2017Imaging spin diffusion in germanium at room temperaturecitations
- 2016Spin Hall effect in AuW alloys
- 2014Electric-field assisted depinning and nucleation of magnetic domain walls in FePt/Al2O3/liquid gate structurescitations
- 2014Electric-field assisted depinning and nucleation of magnetic domain walls in FePt/Al2O3/liquid gate structurescitations
- 2007Electric field-induced modification of magnetism in thin-film ferromagnetscitations
- 2006High-Curie-temperature ferromagnetism in self-organized GeMn nanocolumns
Places of action
| Organizations | Location | People |
|---|
article
Atomic‐Layer Controlled Transition from Inverse Rashba–Edelstein Effect to Inverse Spin Hall Effect in 2D PtSe<sub>2</sub> Probed by THz Spintronic Emission
Abstract
<jats:title>Abstract</jats:title><jats:p>2D materials, such as transition metal dichalcogenides, are ideal platforms for spin‐to‐charge conversion (SCC) as they possess strong spin–orbit coupling (SOC), reduced dimensionality and crystal symmetries as well as tuneable band structure, compared to metallic structures. Moreover, SCC can be tuned with the number of layers, electric field, or strain. Here, SCC in epitaxially grown 2D PtSe<jats:sub>2</jats:sub> by THz spintronic emission is studied since its 1T crystal symmetry and strong SOC favor SCC. High quality of as‐grown PtSe<jats:sub>2</jats:sub> layers is demonstrated, followed by in situ ferromagnet deposition by sputtering that leaves the PtSe<jats:sub>2</jats:sub> unaffected, resulting in well‐defined clean interfaces as evidenced with extensive characterization. Through this atomic growth control and using THz spintronic emission, the unique thickness‐dependent electronic structure of PtSe<jats:sub>2</jats:sub> allows the control of SCC. Indeed, the transition from the inverse Rashba–Edelstein effect (IREE) in 1–3 monolayers (ML) to the inverse spin Hall effect (ISHE) in multilayers (>3 ML) of PtSe<jats:sub>2</jats:sub> enabling the extraction of the perpendicular spin diffusion length and relative strength of IREE and ISHE is demonstrated. This band structure flexibility makes PtSe<jats:sub>2</jats:sub> an ideal candidate to explore the underlying mechanisms and engineering of the SCC as well as for the development of tuneable THz spintronic emitters.</jats:p>