2021
DOI: 10.1016/j.vacuum.2021.110528
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In situ optical and electrical analysis of transient plasmas generated by ns-laser ablation for Ag nanostructured film production

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Cited by 12 publications
(6 citation statements)
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“…Bi plasma is characterized by a narrow range of velocities of the ion structures (1st structure—21 km/s, 2nd structure—8 km/s, 3rd structure—1.5 km/s) and a dominant peak around 1–2 km/s which, according to the work of [ 4 , 34 , 35 ] can be correlated with a nanoparticle (NP) dominated structure. We have confirmed the nature of this slow structure in a recent paper [ 24 ] where we investigated the deposition of Ag nanoparticles by PLD. The widest distribution with ions having velocities up to 60 km/s is the Co plasma defined by low atomic mass particles which can gain more kinetic energy during the acceleration in the initial stages of ablation.…”
Section: Resultssupporting
confidence: 79%
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“…Bi plasma is characterized by a narrow range of velocities of the ion structures (1st structure—21 km/s, 2nd structure—8 km/s, 3rd structure—1.5 km/s) and a dominant peak around 1–2 km/s which, according to the work of [ 4 , 34 , 35 ] can be correlated with a nanoparticle (NP) dominated structure. We have confirmed the nature of this slow structure in a recent paper [ 24 ] where we investigated the deposition of Ag nanoparticles by PLD. The widest distribution with ions having velocities up to 60 km/s is the Co plasma defined by low atomic mass particles which can gain more kinetic energy during the acceleration in the initial stages of ablation.…”
Section: Resultssupporting
confidence: 79%
“…The authors concluded that the low atomic mass elements have a wider angular distribution, results confirmed in [ 17 ] when the ablation of a complex multi-element target was investigated. In recent years Anoop et al [ 18 , 19 , 20 ] and our group [ 21 , 22 , 23 , 24 , 25 , 26 ] used extensive diagnostic investigations on metallic plasma and revealed clear dependence of some plasma parameters on the melting point, atomic mass, or electrical conductivity of the material. The reports are general and cover several irradiation regimes (fs, ps, ns) and a wide range of materials (Al, Cu, Mn, Ni, In, Te, W, Zn, Ti).…”
Section: Introductionmentioning
confidence: 99%
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“…The three-parametric dependence will also be reflected in the expansion velocities of the plasma. As reported by our group in [31][32][33][34], the inner structure of the plasma can have a complex of two or more substructures which forms during expansion. Comparing the geometries of the two plasmas during the deposition process, we observ that the C1 plasma has a more elongated shape reaching the substrate (visible emission contribution to the understanding of the plasma volume) after 500 ns, whereas C2 takes approximately 1 µs having a more compact shape in the first stage of expansion.…”
Section: Real-time Monitoring During Pld Of Ceramic Protective Layermentioning
confidence: 65%