2012
DOI: 10.1063/1.3679103
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Ultraviolet and infrared femtosecond laser induced periodic surface structures on thin polymer films

Abstract: This work demonstrates the formation of femtosecond laser induced periodic surface structures (LIPSS) by multipulse irradiation with the fundamental and 3rd harmonic of a linearly polarized Ti:sapphire laser (795 and 265 nm) on thin films of the polymers poly (ethylene terephthalate), poly (trimethylene terephthalate), and poly (carbonate bisphenol A) prepared by spin-coating. LIPSS, inspected by atomic force microscopy, are formed upon multiple pulse UV and IR irradiation with wavelength-sized period in a nar… Show more

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Cited by 76 publications
(70 citation statements)
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“…In fact, the AFM analysis of the boundary between a non-irradiated and an irradiated area shows that the peaks and valleys of the ripples lie, respectively, above and below the initial surface level. 15 The height of the untreated surface is equivalent to the average height of the nanostructured region of the polymer film, thus confirming that the amount of material removed during laser irradiation is negligible and that the structures originate from a self-organization process not involving ablation. .…”
Section: Afmmentioning
confidence: 68%
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“…In fact, the AFM analysis of the boundary between a non-irradiated and an irradiated area shows that the peaks and valleys of the ripples lie, respectively, above and below the initial surface level. 15 The height of the untreated surface is equivalent to the average height of the nanostructured region of the polymer film, thus confirming that the amount of material removed during laser irradiation is negligible and that the structures originate from a self-organization process not involving ablation. .…”
Section: Afmmentioning
confidence: 68%
“…Values obtained for both 795 and 265 nm at the fluences used for LIPSS formation 15 are well above the unity, indicative of a MP ionization mechanism governing the initial light absorption step. The generation of quasi-free electrons at the early stages of the interaction with the laser pulse has been reported in the case of polymers.…”
Section: à2mentioning
confidence: 83%
“…This means that at least in the beginning of structure formation its period is shorter than the incident light wavelength, as observed experimentally. 26 One can see also that the maximum growth rate for k L ¼ 795 nm is lower by a factor 20 than that for k L ¼ 265 nm. Assuming that the surface structure amplitude is proportional to the growth rate, we may conclude surface structure generation with k L ¼ 795 nm requires about 20 times higher fluence than that with k L ¼ 265 nm, which is also consistent with available experimental data.…”
mentioning
confidence: 83%
“…Assuming that the surface structure amplitude is proportional to the growth rate, we may conclude surface structure generation with k L ¼ 795 nm requires about 20 times higher fluence than that with k L ¼ 265 nm, which is also consistent with available experimental data. 26 It is worth pointing out that LIMIS with pulsed excitation as illustrated in Fig. 4 is quite high even for relatively high heat conductance and low thermal expansion.…”
mentioning
confidence: 99%
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