PMID- 30968864 OWN - NLM STAT- PubMed-not-MEDLINE LR - 20191120 IS - 1364-5528 (Electronic) IS - 0003-2654 (Linking) VI - 144 IP - 10 DP - 2019 May 13 TI - Effect of energy per atom (E/n) on the Ar gas cluster ion beam (Ar-GCIB) and O(2)(+) cosputter process. PG - 3323-3333 LID - 10.1039/c8an02452a [doi] AB - Gas cluster ion beam (GCIB) is a promising technique for preserving molecular structures during ion sputtering and successfully profiling biological and soft materials. However, although GCIB yields lower damage accumulation compared with C60+ and monoatomic ion beams, the inevitable alteration of the chemical structure can introduce artifacts into the resulting depth profile. To enhance the ionization yield and further mask damage, a low-energy O2+ (200-500 V) cosputter can be applied. While the energy per atom (E/n) of GCIB is known to be an important factor influencing the sputter process, the manner through which E/n affects the GCIB-O2+ cosputter process remains unclear. In this study, poly(ethylene terephthalate) (PET) was used as a model material to investigate the sputter process of 10-20 kV Ar1000-4000+ (E/n = 2.5-20 eV per atom) with and without O2+ cosputter at different energies and currents. Time-of-flight secondary ion mass spectrometry (ToF-SIMS) with Bi32+ as the primary ion was used to examine surfaces sputtered at different fluences. The sputter craters were also measured by alpha-step and atomic force microscopy in quantitative imaging mode. The SIMS results showed that the steady-state cannot be obtained with E/n values of less than 5 eV per atom due to damage accumulation using single GCIB sputtering. With a moderate E/n value of 5-15 eV per atom, the steady-state can be obtained, but the approximately 50% decay in intensity indicated that damage cannot be masked completely despite the higher sputter yield. Furthermore, the surface Young's modulus decreased with increasing E/n, suggesting that depolymerization occurred. At an E/n value of 20 eV per atom, a failed profile was obtained with rapidly decreased sputter rate and secondary ion intensity due to the ion-induced crosslink. With O2+ cosputtering and a moderate E/n value, the oxidized species generated by O2+ enhanced the ionization yield, which led to a higher ion intensity at steady-state in general. Because higher kinetic energy or current density of O2+ led to a larger interaction volume and more structural damage that suppressed molecular ion intensity, the enhancement from O2+ was most apparent with low-energy-high-current (200 V, 80 muA cm-2) or high-energy-low-current (500 V, 5 muA cm-2) O2+ cosputtering with 0.5 muA cm-2 GCIBs. In these cases, little or no intensity drop was observed at the steady-state. FAU - Wang, Shin-Kung AU - Wang SK AD - Department of Materials Science and Engineering, National Taiwan University, Taipei 106, Taiwan. shyue@gate.sinica.edu.tw. FAU - Chang, Hsun-Yun AU - Chang HY FAU - Chu, Yi-Hsuan AU - Chu YH FAU - Kao, Wei-Lun AU - Kao WL FAU - Wu, Chen-Yi AU - Wu CY FAU - Lee, Yi-Wei AU - Lee YW FAU - You, Yun-Wen AU - You YW FAU - Chu, Kuo-Jui AU - Chu KJ FAU - Hung, Shu-Hang AU - Hung SH FAU - Shyue, Jing-Jong AU - Shyue JJ LA - eng PT - Journal Article PL - England TA - Analyst JT - The Analyst JID - 0372652 EDAT- 2019/04/11 06:00 MHDA- 2019/04/11 06:01 CRDT- 2019/04/11 06:00 PHST- 2019/04/11 06:00 [pubmed] PHST- 2019/04/11 06:01 [medline] PHST- 2019/04/11 06:00 [entrez] AID - 10.1039/c8an02452a [doi] PST - ppublish SO - Analyst. 2019 May 13;144(10):3323-3333. doi: 10.1039/c8an02452a.