| Autor: |
Pliatsikas N; Department of Physics, Aristotle University of Thessaloniki, GR-54124 Thessaloniki, Greece., Panos S; Department of Physics, Aristotle University of Thessaloniki, GR-54124 Thessaloniki, Greece., Odutola T; Department of Physics, Aristotle University of Thessaloniki, GR-54124 Thessaloniki, Greece., Kassavetis S; Department of Physics, Aristotle University of Thessaloniki, GR-54124 Thessaloniki, Greece., Papoulia C; Department of Physics, Aristotle University of Thessaloniki, GR-54124 Thessaloniki, Greece., Fekas I; Department of Physics, Aristotle University of Thessaloniki, GR-54124 Thessaloniki, Greece., Arvanitidis J; Department of Physics, Aristotle University of Thessaloniki, GR-54124 Thessaloniki, Greece., Christofilos D; School of Chemical Engineering and Physics Laboratory, Faculty of Engineering, Aristotle University of Thessaloniki, GR-54124 Thessaloniki, Greece., Pavlidou E; Department of Physics, Aristotle University of Thessaloniki, GR-54124 Thessaloniki, Greece., Gioti M; Department of Physics, Aristotle University of Thessaloniki, GR-54124 Thessaloniki, Greece., Patsalas P; Department of Physics, Aristotle University of Thessaloniki, GR-54124 Thessaloniki, Greece. |
| Abstrakt: |
Titanium nitride (TiN) is a candidate material for several plasmonic applications, and pulsed laser ablation in liquids (PLAL) represents a rapid, scalable, and environmentally friendly approach for the large-scale production of nanomaterials with customized properties. In this work, the nanosecond PLAL process is developed, and we provide a concise understanding of the process parameters, such as the solvent and the laser fluence and pulse wavelength, to the size and structure of the produced TiN nanoparticles (NPs). TiN films of a 0.6 μm thickness developed by direct-current (DC) magnetron sputtering were used as the ablation targets. All laser process parameters lead to the fabrication of spherical NPs, while the laser pulse fluence was used to control the NPs' size. High laser pulse fluence values result in larger TiN NPs (diameter around 42 nm for 5 mJ and 25 nm for 1 mJ), as measured from scanning electron microscopy (SEM). On the other hand, the wavelength of the laser pulse does not affect the mean size of the TiN NPs (24, 26, and 25 nm for 355, 532, and 1064 nm wavelengths, respectively). However, the wavelength plays a vital role in the quality of the produced TiN NPs. Shorter wavelengths result in NPs with fewer defects, as indicated by Raman spectra and XPS analysis. The solvent type also significantly affects the size of the NPs. In aqueous solutions, strong oxidation of the NPs is evident, while organic solvents such as acetone, carbides, and oxides cover the TiN NPs. |
