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Molecular dynamic‐secondary ion mass spectrometry (D‐SIMS) ionized by co‐sputtering with C 60 + and Ar
Dynamic secondary ion mass spectrometry (D‐SIMS) analysis of poly(ethylene terephthalate) (PET) and poly(methyl methacrylate) (PMMA) was conducted using a quadrupole mass analyzer with various combinations of continuous C 60 + and Ar + ion sputtering. Individually, the Ar + beam failed to generate f...
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Published in: | Rapid communications in mass spectrometry 2011-10, Vol.25 (19), p.2897-2904 |
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Main Authors: | , , , , , , , , , , , |
Format: | Article |
Language: | English |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | Dynamic secondary ion mass spectrometry (D‐SIMS) analysis of poly(ethylene terephthalate) (PET) and poly(methyl methacrylate) (PMMA) was conducted using a quadrupole mass analyzer with various combinations of continuous C
60
+
and Ar
+
ion sputtering. Individually, the Ar
+
beam failed to generate fragments above
m
/
z
200, and the C
60
+
beam generated molecular fragments of
m
/
z
~1000. By combining the two beams, the auxiliary Ar
+
beam, which is proposed to suppress carbon deposition due to C
60
+
bombardment and/or remove graphitized polymer, the sputtering range of the C
60
+
beam is extended. Another advantage of this technique is that the high sputtering rate and associated high molecular ion intensity of the C
60
+
beam generate adequate high‐mass fragments that mask the damage from the Ar
+
beam. As a result, fragments at
m
/
z
~900 can be clearly observed. As a depth‐profiling tool, the single C
60
+
beam cannot reach a steady state for either PET or PMMA at high ion fluence, and the intensity of the molecular fragments produced by the beam decreases with increasing C
60
+
fluence. As a result, the single C
60
+
beam is suitable for profiling surface layers with limited thickness. With C
60
+
‐Ar
+
co‐sputtering, although the initial drop in intensity is more significant than with single C
60
+
ionization because of the damage introduced by the auxiliary Ar
+
, the intensity levels indicate that a more steady‐state process can be achieved. In addition, the secondary ion intensity at high fluence is higher with co‐sputtering. As a result, the sputtered depth is enhanced with co‐sputtering and the technique is suitable for profiling thick layers. Furthermore, co‐sputtering yields a smoother surface than single C
60
+
sputtering. Copyright © 2011 John Wiley & Sons, Ltd. |
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ISSN: | 0951-4198 1097-0231 |
DOI: | 10.1002/rcm.5181 |