2018
DOI: 10.1007/s00339-018-1714-2
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Effects of pulse durations and environments on femtosecond laser ablation of stainless steel

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Cited by 24 publications
(14 citation statements)
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“…Bizi-bandoki P. et al [36] prepared porous and splashlike structures in the central ablation region at a higher laser fluence (more than 3.31 J/cm 2 ) and number of pulses (more than 70), and the microscale holes were arranged in an orderly circle, as shown in Figure 7. Similar structures were obtained by Maharjan N. and Xu S. [39,47].…”
Section: Other Structuressupporting
confidence: 85%
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“…Bizi-bandoki P. et al [36] prepared porous and splashlike structures in the central ablation region at a higher laser fluence (more than 3.31 J/cm 2 ) and number of pulses (more than 70), and the microscale holes were arranged in an orderly circle, as shown in Figure 7. Similar structures were obtained by Maharjan N. and Xu S. [39,47].…”
Section: Other Structuressupporting
confidence: 85%
“…Bizi-bandoki P. et al [36] found that nanoscale LSFL structures were sensitive only to the number of pulses, with a 15% reduction in the structure period as the number of pulses increased. Yao C., Xu S. and Yasumaru N. [32,47,48] obtained similar influence laws, with the ripple period decreasing with the number of pulses or the number of scans.…”
Section: Pulse Number/scan Numbermentioning
confidence: 75%
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“…With temporal pulse lengths <10 ps in ultrafast laser ablation, the instantaneous energy deposition reduces plasma absorption while minimizing melt and thermal diffusion during the pulse and yield high precision material removal [ 13 , 14 ]. This allows for easy generation of plasmonic, interferometric and hierarchical microstructures on, for example, stainless steel [ 15 , 16 , 17 ]. In metals, which have absorption coefficients typically α ~10 6 cm −1 , a thin layer with thickness d ~10–30 nm is converted to a plasma at a solid density which expands well after the pulse is absorbed [ 18 , 19 ].…”
Section: Introductionmentioning
confidence: 99%