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A study on selective surface nitridation of TiO 2 nanocrystals in the afterglows of N 2 and N 2 -O 2 microwave plasmas
  • Jeon, Byungwook ;
  • Kim, Ansoon ;
  • Ricard, André ;
  • Sarrette, Jean Philippe ;
  • Yu, Xiaomei ;
  • Kim, Yu Kwon
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Publication Year
2018-02-28
Publisher
Elsevier B.V.
Citation
Applied Surface Science, Vol.432, pp.163-169
Keyword
AfterglowMicrowave plasmaN 2Surface modificationTiO 2
Mesh Keyword
AfterglowChemical bonding stateExposure conditionsMicrowave plasmaSelective surfaceTiO2TiO2 nanocrystalsX ray photoemission spectroscopy
All Science Classification Codes (ASJC)
Condensed Matter PhysicsSurfaces and InterfacesSurfaces, Coatings and Films
Abstract
Surface-selective chemical modification of anatase TiO 2 nanocrystals is performed in the post-discharge region of N 2 microwave plasma and the chemical bonding states of surface nitrogen species are carefully evaluated using X-ray photoemission spectroscopy (XPS). It is found that the surface treatments in the afterglows induce the formation of stable nitrogen species at or near the surface of TiO 2 . Interestingly, the detailed bonding structure varies strongly depending on the afterglow condition. In pure N 2 afterglows, various N species with a direct Ti–N bond are formed on the surface, while the use of N 2 -O 2 mixtures induces the formation of additional oxidized species of NO 3 − on the surface. This is attributed to the high concentrations of O or NO in the afterglows of N 2 -O 2 plasmas. The incorporation of substitutional N species in the subsurface is also achieved after a prolonged exposure in the early afterglow with a high density of N 2 + species. Our results show that the exposure condition can be controlled for a selective chemical modification of TiO 2 surface for the control of surface properties in various applications.
ISSN
0169-4332
Language
eng
URI
https://dspace.ajou.ac.kr/dev/handle/2018.oak/29993
DOI
https://doi.org/10.1016/j.apsusc.2017.07.113
Fulltext

Type
Article
Funding
This research was supported by the International Research & Development Program of the National Research Foundation of Korea (NRF) funded by the Ministry of Science, ICT & Future Planning ( NRF-2015K1A3A1A21000248 ). This work was also supported by the Human Resources Development of the Korea Institute of Energy Technology Evaluation and Planning (KETEP) grant funded by the Korea government Ministry of Trade, industry & Energy (No. 20154010200820 ). AR and JPS would like to thank for its support the Ministry of Foreign Affairs and of International Development through the PHC STAR grant 34306TK . Appendix A
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