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SiO2 etching in inductively coupled plasmas using heptafluoroisopropyl methyl ether and 1,1,2,2-tetrafluoroethyl 2,2,2-trifluoroethyl ether
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Publication Year
2020-04-01
Publisher
Elsevier B.V.
Citation
Applied Surface Science, Vol.508
Keyword
Angular dependenceEtch yieldFaraday cageSiO2 etchingSteady-state fluorocarbon film
Mesh Keyword
Angular dependenceEtch yieldFaraday cageFluorocarbon filmsGlobal warming potentialIon incidence anglePerfluorocompoundsSubstrate surface
All Science Classification Codes (ASJC)
Chemistry (all)Condensed Matter PhysicsPhysics and Astronomy (all)Surfaces and InterfacesSurfaces, Coatings and Films
Abstract
Heptafluoroisopropyl methyl ether (HFE-347mmy) and 1,1,2,2-tetrafluoroethyl 2,2,2-trifluoroethyl ether (HFE-347pcf2), whose global warming potentials are significantly lower than those of perfluorocompounds, are used for plasma etching of SiO2. The SiO2 etch rates are higher in the HFE-347mmy/Ar plasma than in the HFE-pcf2/Ar plasma owing to the larger production of CF2 radicals and corresponding formation of thicker fluorocarbon films on the substrate surface in the HFE-347pcf2/Ar plasma than in the HFE-347mmy/Ar plasma. The angular dependences of the etch rates at various bias voltages (−400 to −1200 V) are measured using a Faraday cage. The normalized etch yields (NEYs) have the maxima at ion incidence angles between 50° and 60° in both plasmas at all bias voltages. The NEYs increase with the bias voltage up to −800 V, and then virtually follow a single curve for bias voltages higher than −800 V in HFE-347mmy/Ar, while they continuously increase with the bias voltage in the range of −400 to −1200 V in HFE-347pcf2/Ar. The dependences of the NEYs of SiO2 on the ion incidence angle and bias voltage in both plasmas are explained by analyzing the thicknesses and fluorine-to-carbon ratios of the steady-state fluorocarbon films formed on the substrate surfaces.
ISSN
0169-4332
Language
eng
URI
https://dspace.ajou.ac.kr/dev/handle/2018.oak/31047
DOI
https://doi.org/10.1016/j.apsusc.2019.144787
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Type
Article
Funding
This work was supported by the Korea Institute of Energy Technology Evaluation and Planning (KETEP) grant funded by the Korea Government Ministry of Trade, Industry and Energy (Grant No. 20172010104830 ), the National Research Foundation of Korea (NRF) grant funded by the Korea government (MEST) (grant No. 2018R1A2B6002410 ), and the GRRC program of Gyeonggi province ( GRRC AJOU 2016B03 , Photonics-Medical Convergence Technology Research Center ).This work was supported by the Korea Institute of Energy Technology Evaluation and Planning (KETEP) grant funded by the Korea Government Ministry of Trade, Industry and Energy (Grant No. 20172010104830), the National Research Foundation of Korea (NRF) grant funded by the Korea government (MEST) (grant No. 2018R1A2B6002410), and the GRRC program of Gyeonggi province (GRRC AJOU 2016B03, Photonics-Medical Convergence Technology Research Center).
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Kim, Chang-Koo Image
Kim, Chang-Koo김창구
Department of Chemical Engineering
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