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In Plasma ion beam analysis of polymer layer and adsorbed H monolayer etching

We present two experiments where a layer is plasma-etched while monitoring its evolution by in plasma ion beam analysis. First, we etch a photoresist with a diffuse O2 plasma at low pressure. Using a 4.335 MeV He beam, Rutherford Backscattering Spectrometry and Elastic Recoil Detection spectra are a...

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Published in:Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms Beam interactions with materials and atoms, 2024-09, Vol.554, p.165439, Article 165439
Main Authors: Fortier, Louis-Charles, Chicoine, Martin, Chouteau, Simon, Clausse, Mathilde, Lalande, Émile, Lussier, Alexandre W., Roorda, Sjoerd, Stafford, Luc, Terwagne, Guy, Schiettekatte, François
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container_title Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms
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creator Fortier, Louis-Charles
Chicoine, Martin
Chouteau, Simon
Clausse, Mathilde
Lalande, Émile
Lussier, Alexandre W.
Roorda, Sjoerd
Stafford, Luc
Terwagne, Guy
Schiettekatte, François
description We present two experiments where a layer is plasma-etched while monitoring its evolution by in plasma ion beam analysis. First, we etch a photoresist with a diffuse O2 plasma at low pressure. Using a 4.335 MeV He beam, Rutherford Backscattering Spectrometry and Elastic Recoil Detection spectra are acquired every minute during 8 h. Etching of most elements follows a linear trend, but H desorbs faster at the beginning of the plasma process, which we ascribe to the ion beam-induced desorption. In addition, we observe a thin Mo layer building up at the surface, likely due to the sputtering of an electrode in the plasma source. Secondly, we etch in HF a crystalline Si (c-Si) sample with surface orientation, which should leave 14 H/nm2 bonded to the c-Si surface. The sample is then introduced in the chamber and exposed to a diffuse Ar plasma at low pressure. During plasma processing, the H surface concentration is monitored using a resonant nuclear reaction with a 15N beam at 6.385 MeV. The initial H concentration is 11.7±1.1 H/nm2, and it decreases over a 3-minute timescale to an equilibrium concentration of 6.0±0.8 H/nm2. Over the range of experimental conditions investigated, the diffuse Ar plasma is therefore not able to entirely sputter the H from the c-Si surface.
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subjects ERD
In plasma
Ion beam analysis
NRRA
Plasma etching
RBS
title In Plasma ion beam analysis of polymer layer and adsorbed H monolayer etching
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