2016
DOI: 10.1016/j.apsusc.2016.03.008
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Femtosecond laser nanostructuring of titanium metal towards fabrication of low-reflective surfaces over broad wavelength range

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Cited by 51 publications
(36 citation statements)
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“…FLSP can be used to create low reflectivity, high absorption surfaces for light with wavelengths from ultraviolet to terahertz radio waves. [33][34][35][36] Such optoelectronic properties can be used for solar thermal energy conversion, molecular spectroscopy, plasmonics, and stealth technologies. Recently, FLSP of Ti has been shown to improve wear for tribological applications.…”
Section: Introductionmentioning
confidence: 99%
“…FLSP can be used to create low reflectivity, high absorption surfaces for light with wavelengths from ultraviolet to terahertz radio waves. [33][34][35][36] Such optoelectronic properties can be used for solar thermal energy conversion, molecular spectroscopy, plasmonics, and stealth technologies. Recently, FLSP of Ti has been shown to improve wear for tribological applications.…”
Section: Introductionmentioning
confidence: 99%
“…A large amount of UHSFLs of 30–50 nm per period are located in the troughs and joint regions of LSFLs/HSFLs. The periods of UHSFLs are much narrower than those prepared on Ti by fs-LA in air [ 27 , 28 , 29 ]. In a relatively deeper trough of LSFLs/HSFLs, UHSFLs are characterized by extra stretched nanowires from their middle parts (pointed out by green arrows in Figure 1 e), so that it is difficult to differentiate them from main UHSFLs ( Figure 1 e).…”
Section: Resultsmentioning
confidence: 99%
“…Recently, our group has shown the necessity to define sub-100 nm [ 17 , 18 , 19 , 20 ] periods as a new category of ultrahigh spatial frequency LIPSSs (UHSFLs) because (1) UHSFLs whose periods are as small as 40 nm [ 17 , 21 ] are very difficult to form on semiconductors (so far, only two reports on Si) when compared with normal HSFLs with periods in the range of 100–200 nm [ 15 , 22 , 23 ]; (2) The periods of UHSFLs prepared on metals are much smaller than normal HSFLs with periods of hundreds of nm [ 24 , 25 , 26 ]. For example, Bosen et al prepared homogeneous UHSFLs (periods: 70–90 nm) on Ti by fs-LA in air (λ = 790 nm, τ = 30–160 fs and υ = 1 kHz) [ 27 , 28 , 29 ] and found that such fine structures can be easily destroyed during the friction tests in two different lubricating oils [ 30 ]. Sedao et al revealed the role of surface melting and resolidification in the formation of UHSFLs of 70–90 nm in a period on Ni [ 31 ].…”
Section: Introductionmentioning
confidence: 99%
“…It is known that during normal incidence of femtosecond, linearly polarized laser pulses, low-spatial-frequency laser-induced periodic surface structures (LSFL) are formed on the copper surface, which demonstrate the effect of diffraction staining [25,26]. That is, the appearance of a surface relief demonstrating properties of a diffraction grating in the visible range is observed.…”
Section: Results Of Experimental Studiesmentioning
confidence: 99%