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dc.contributor.authorVinchon, Pierre
dc.contributor.authorAsadollahi, Siavash
dc.contributor.authorCoté, Claude
dc.contributor.authorMarcet, Stephane
dc.contributor.authorAtallah, S.
dc.contributor.authorDessureault, Émile
dc.contributor.authorChicoine, Martin
dc.contributor.authorSarkissian, Andranik
dc.contributor.authorLeonelli, Richard
dc.contributor.authorRoorda, Sjoerd
dc.contributor.authorSchiettekatte, François
dc.contributor.authorStafford, Luc
dc.date.accessioned2024-03-19T17:17:02Z
dc.date.availableNO_RESTRICTIONfr
dc.date.available2024-03-19T17:17:02Z
dc.date.issued2023
dc.identifier.urihttp://hdl.handle.net/1866/32803
dc.publisherAmerican Institute of Physicsfr
dc.subjectPlasma processingfr
dc.subjectGraphenefr
dc.subjectRaman spectroscopyfr
dc.subjectIon beam analysisfr
dc.subjectRutherford backscattering spectrometryfr
dc.subjectPlasma material interactionsfr
dc.subjectPlasma sourcesfr
dc.titleIn-plasma analysis of plasma–surface interactionsfr
dc.typeArticlefr
dc.contributor.affiliationUniversité de Montréal. Faculté des arts et des sciences. Département de physiquefr
dc.identifier.doi10.1063/5.0130235
dcterms.abstractDuring deposition, modification, and etching of thin films and nanomaterials in reactive plasmas, many active species can interact with the sample simultaneously. This includes reactive neutrals formed by fragmentation of the feed gas, positive ions, and electrons generated by electron-impact ionization of the feed gas and fragments, excited states (in particular, long-lived metastable species), and photons produced by spontaneous de-excitation of excited atoms and molecules. Notably, some of these species can be transiently present during the different phases of plasma processing, such as etching of thin layer deposition. To monitor plasma–surface interactions during materials processing, a new system combining beams of neutral atoms, positive ions, UV photons, and a magnetron plasma source has been developed. This system is equipped with a unique ensemble of in-plasma surface characterization tools, including (1) a Rutherford Backscattering Spectrometer (RBS), (2) an Elastic Recoil Detector (ERD), and (3) a Raman spectroscopy system. RBS and ERD analyses are carried out using a differentially pumped 1.7 MV ion beam line Tandetron accelerator generating a beam at grazing incidence. The ERD system is equipped with an absorber and is specifically used to detect H initially bonded to the surface; higher resolution of surface H is also available through nuclear reaction analysis. In parallel, an optical port facing the substrate is used to perform Raman spectroscopy analysis of the samples during plasma processing. This system enables fast monitoring of a few Raman peaks over nine points scattered on a 1.6 × 1.6 mm2 surface without interference from the inherent light emitted by the plasma. Coupled to the various plasma and beam sources, the unique set of in-plasma surface characterization tools detailed in this study can provide unique time-resolved information on the modification induced by plasma. By using the ion beam analysis capability, the atomic concentrations of various elements in the near-surface (e.g., stoichiometry and impurity content) can be monitored in real-time during plasma deposition or etching. On the other hand, the evolution of Raman peaks as a function of plasma processing time can contribute to a better understanding of the role of low-energy ions in defect generation in irradiation-sensitive materials, such as monolayer graphene.fr
dcterms.isPartOfurn:ISSN:0034-6748fr
dcterms.isPartOfurn:ISSN:1089-7623fr
dcterms.languageengfr
UdeM.ReferenceFournieParDeposanthttps://doi.org/10.1063/5.0130235fr
UdeM.VersionRioxxVersion acceptée / Accepted Manuscriptfr
oaire.citationTitleReview of scientific instrumentsfr
oaire.citationVolume94fr


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