4.6 Article

Femtosecond laser-induced periodic surface structures on diamond-like nanocomposite films

Journal

DIAMOND AND RELATED MATERIALS
Volume 130, Issue -, Pages -

Publisher

ELSEVIER SCIENCE SA
DOI: 10.1016/j.diamond.2022.109517

Keywords

Diamond -like nanocomposite (DLN) films; Femtosecond laser ablation; Spallation; Laser -induced periodic surface structures; (LIPSS); Graphitization; Raman spectroscopy; Ti-doped DLN films

Funding

  1. Russian Science Foundation
  2. [15-12-00039]

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This study focuses on the formation of high and low spatial frequency laser-induced periodic surface structures (LIPSS) on DLN and Ti-DLN films using femtosecond laser ablation. The effects of different laser parameters and film properties on the LIPSS formation are investigated. The presence of plasmonic effects, such as the superposition of high and low frequency LIPSS and the emergence of sinusoid-like structures, are discussed.
We study the formation of laser-induced periodic surface structures (LIPSS) on diamond-like nanocomposite (DLN) a-C:H:Si:O films and titanium-doped DLN films during femtosecond (fs) laser ablation processing with linearly-polarized beams of IR and visible fs-lasers (wavelengths 1030 nm and 515 nm, pulse duration 320 fs, pulse repetition rates 100 kHz-2 MHz, scanning beam velocity 0.04-0.4 m/s). The studies are focused on (i) comparison of high spatial frequency LIPSS (HSFL) and low spatial frequency LIPSS (LSFL) formed on DLN and Ti-DLN films by IR fs-laser processing, (ii) effects of the pulse repetition rate on the parameters of LIPSS formed on the DLN and Ti-DLN films, (iii) Raman spectroscopy analysis of the LIPSS-structured films with application for ultrathin surface graphitization, and (iv) relationship between the fs-laser-induced surface graphitization and LIPSS formation on the films. A variety of the HSFL and LSFL have been produced on the surface of DLN and TiDLN films, with all the LIPSS being oriented perpendicular to the beam polarization direction. The HSFL periods are varied from -80 to 240 nm and the LSFL periods are varied from 355 to 840 nm, depending on the fs-laser irradiation conditions (wavelength, fluence, pulse repetition rate) and films properties. Various plasmonic effects such as the superposition of the HSFL and LSFL and emergence of very unusual sinusoid-like structures on the DLN and Ti-DLN films are presented and discussed.

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