1997
DOI: 10.1016/s0039-6028(97)00397-x
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Morphology of sputtering damage on Cu(111) studied by scanning tunneling microscopy

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Cited by 32 publications
(19 citation statements)
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“…1 and 2 is the extreme similarity of the entire ethene spectra for the two different defective Cu͑111͒ surfaces. In general, sputtering is not equivalent to a sort of "negative" deposit where adislands are replaced by vacancies [33][34][35] because the mobility of adatom clusters may be larger than the one of vacancy clusters. 26,[36][37][38] The similarity of the vibrational losses of ethene ͑the difference in the frequencies being smaller than Ϯ3 meV͒ allows us to conclude that as far as ethene adsorption is concerned, it does not matter how the surface roughness was induced.…”
Section: A Assignment Of the Lossesmentioning
confidence: 99%
“…1 and 2 is the extreme similarity of the entire ethene spectra for the two different defective Cu͑111͒ surfaces. In general, sputtering is not equivalent to a sort of "negative" deposit where adislands are replaced by vacancies [33][34][35] because the mobility of adatom clusters may be larger than the one of vacancy clusters. 26,[36][37][38] The similarity of the vibrational losses of ethene ͑the difference in the frequencies being smaller than Ϯ3 meV͒ allows us to conclude that as far as ethene adsorption is concerned, it does not matter how the surface roughness was induced.…”
Section: A Assignment Of the Lossesmentioning
confidence: 99%
“…While Zhou and Wadley did not address re-sputtering effects above 50 eV, it is clear that sputter yields increase quickly above 50 eV. In work done on Pt(111) (whose atomistics are similar to Cu(111) [12]) sputter and adatom/vacancy yields of 1 were observed at 200 eV for Xe + [13]. This suggests that the dramatic morphological change between 60 eV and 100 eV in Figure 1 is due to the onset of sputter erosion.…”
Section: Discussionmentioning
confidence: 99%
“…DIS experiments were performed at the Radiation Surface Science and Engineering Laboratory (RSSEL) in the School of Nuclear Engineering, Purdue University, in the Particle and Radiation Interaction with Soft and Hard Matter (PRIHSM) facility, originally developed and operated by Prof. Jean Paul Allain at Purdue University [27]. DIS conditions are summarized in Table 1; Energy, fluence, and incidence angle were chosen after an exhaustive revision of our previous DIS nano-structuring results on metallic materials [33,34], as well as from some other revised works on Ti, TiO 2 , Cu, Au, and Ag [35][36][37][38][39][40][41][42][43][44][45]. Argon (Ar + ) source at 1 and 0.5 keV was used to irradiate PPS samples and NPS; the selection of DIS parameters were designed to evaluate their effect on nanopatterning.…”
Section: Directed Irradiation Synthesis (Dis) Of Porous and Non-poroumentioning
confidence: 99%