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 |
|
Hagen, Cornelis Wouter
Delft University of Technology
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (7/7 displayed)
- 2024Water-assisted purification during electron beam-induced deposition of platinum and goldcitations
- 2022Ultra-thin corrugated metamaterial film as large-area transmission dynodecitations
- 2021Secondary electron emission from multi-layered TiN/Al2O3transmission dynodescitations
- 2021Mechanical characterization of nanopillars by atomic force microscopycitations
- 2020‘Cleanroom’ in SEMcitations
- 2020Electron beam-induced deposition of platinum from Pt(CO)2Cl2 and Pt(CO)2Br2citations
- 2017Electron transport and room temperature single-electron charging in 10 nm scale PtC nanostructures formed by electron beam induced depositioncitations
Places of action
Organizations | Location | People |
---|
article
Ultra-thin corrugated metamaterial film as large-area transmission dynode
Abstract
<p>Large-area transmission dynodes were fabricated by depositing an ultra-thin continuous film on a silicon wafer with a 3-dimensional pattern. After removing the silicon, a corrugated membrane with enhanced mechanical properties was formed. Mechanical metamaterials, such as this corrugated membrane, are engineered to improve its strength and robustness, which allows it to span a larger surface in comparison to flat membranes while the film thickness remains constant. The ultra-thin film consists of three layers (Al<sub>2</sub>O<sub>3</sub>/TiN/Al<sub>2</sub>O<sub>3</sub>) and is deposited by atomic layer deposition (ALD). The encapsulated TiN layer provides in-plane conductivity, which is needed to sustain secondary electron emission. Two types of corrugated membranes were fabricated: a hexagonal honeycomb and an octagonal pattern. The latter was designed to match the square pitch of a CMOS pixel chip. The transmission secondary electron yield was determined with a collector-based method using a scanning electron microscope. The highest transmission electron yield was measured on a membrane with an octagonal pattern. A yield of 2.15 was achieved for 3.15 keV incident electrons for an Al<sub>2</sub>O<sub>3</sub>/TiN/Al<sub>2</sub>O<sub>3</sub> tri-layer film with layer thicknesses of 10/5/15 nm. The variation in yield across the surface of the corrugated membrane was determined by constructing a yield map. The active surface for transmission secondary electron emission is near 100%, i.e. a primary electron generates transmission secondary electrons regardless of the point of impact on the corrugated membrane.</p>