2020
DOI: 10.1016/j.procir.2020.09.098
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Generation of Laser-Induced Periodic Surface Structures on Different Glasses by a Picosecond-Pulsed Laser

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Cited by 5 publications
(2 citation statements)
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“…For wavelengths in the range of 300-2000 nm, this requirement is fulfilled trivially for most metals and semiconductors. For dielectric materials it may be necessary to pre-heat the electronic system with a pre-pulse and thus changing the dielectric function [64,65]. At normal incidence, the period of the resulting structures Λ LIPSS is determined by the wavelength of the SPP [66][67][68][69] and can be calculated from the dispersion relation of the SPP 2.58:…”
Section: Surface Plasmon Polariton Theorymentioning
confidence: 99%
See 1 more Smart Citation
“…For wavelengths in the range of 300-2000 nm, this requirement is fulfilled trivially for most metals and semiconductors. For dielectric materials it may be necessary to pre-heat the electronic system with a pre-pulse and thus changing the dielectric function [64,65]. At normal incidence, the period of the resulting structures Λ LIPSS is determined by the wavelength of the SPP [66][67][68][69] and can be calculated from the dispersion relation of the SPP 2.58:…”
Section: Surface Plasmon Polariton Theorymentioning
confidence: 99%
“…Electromagnetic Theories Another electromagnetic theory is based on electromagnetic waves called radiation remnants, that have first been discussed by Sipe et al [74]. This theory is used to describe the phenomenon of LSFL that are found on transparent dielectrics [65,69,75]. This type of LSFL are, in contrast to the LSFL given by the SPP theory, parallel to the polarisation of the laser beam and are therefore sometimes called LSFL || or LSFL-II.…”
Section: Other Theoriesmentioning
confidence: 99%