The role of the auxiliary atomic ion beam in C60+–Ar+co-sputtering
Author(s) -
WeiChun Lin,
ChiPing Liu,
Che-Hung Kuo,
HsunYun Chang,
C. C. Chang,
TungHan Hsieh,
Szu-Hsian Lee,
YunWen You,
WeiLun Kao,
GuoJi Yen,
ChihChieh Huang,
JingJong Shyue
Publication year - 2010
Publication title -
the analyst
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.998
H-Index - 153
eISSN - 1364-5528
pISSN - 0003-2654
DOI - 10.1039/c0an00642d
Subject(s) - sputtering , ion beam , x ray photoelectron spectroscopy , ion , analytical chemistry (journal) , ion beam deposition , chemistry , secondary ion mass spectrometry , mass spectrometry , materials science , atomic physics , thin film , nanotechnology , nuclear magnetic resonance , physics , organic chemistry , chromatography
Cluster ion sputtering has been proven to be an effective technique for depth profiling of organic materials. In particular, C(60)(+) ion beams are widely used to profile soft matter. The limitation of carbon deposition associated with C(60)(+) sputtering can be alleviated by concurrently using a low-energy Ar(+) beam. In this work, the role of this auxiliary atomic ion beam was examined by using an apparatus that could analyze the sputtered materials and the remaining target simultaneously using secondary ion mass spectrometry (SIMS) and X-ray photoelectron spectrometry (XPS), respectively. It was found that the auxiliary 0.2 kV Ar(+) stream was capable of slowly removing the carbon deposition and suppresses the carbon from implantation. As a result, a more steady sputtering condition was achieved more quickly with co-sputtering than by using C(60)(+) alone. Additionally, the Ar(+) beam was found to interfere with the C(60)(+) beam and may lower the overall sputtering rate and secondary ion intensity in some cases. Therefore, the current of this auxiliary ion beam needs to be carefully optimized for successful depth profiling.
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