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Search for "production upscale" in Full Text gives 1 result(s) in Beilstein Journal of Nanotechnology.

Beam shaping techniques for pulsed laser ablation in liquids: Unlocking tunable control of nanoparticle synthesis in liquids

Sergio Molina-Prados,
Nadezhda M. Bulgakova,
Alexander V. Bulgakov,
Jesus Lancis,
Gladys Mínguez Vega and
Carlos Doñate-Buendia

Beilstein J. Nanotechnol. 2026, 17, 309–342, doi:10.3762/bjnano.17.22

highlighted, offering a comprehensive perspective on the future of this dynamic field. Keywords: green nanoparticles synthesis; PLAL; production upscale; pulsed laser ablation in liquids; size control; spatial beam shaping; temporal beam shaping; Review Introduction Pulsed laser ablation in liquids (PLAL

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Figure 1: Comparative analysis of the main features of nanomaterial synthesis techniques, that is, chemical, ...

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Figure 2: PLAL NP applications, arrows point outwards to the four defined areas, catalysis, advanced material...

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Figure 3: Schematic illustration of spatial beam shaping strategies in PLAL. Different beam profiles can be g...

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Figure 4: (a) Experimental setup for the record of filamentation produced in a liquid. (b) Laser focusing in ...

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Figure 5: Top: Ablated spot diameter on a silicon wafer comparison between air and with 10 mm water layer. Bo...

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Figure 6: (a, b) Nanoparticle concentrations, (c, d) hydrodynamic diameters, and (e, f) ξ-potential of one an...

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Figure 7: TEM images of Ag nanoribbons produced by cylindrical lens ablation at a pulse energy of 1.2 mJ. Ag ...

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Figure 8: (a, b) Transverse distributions of Bessel-like beams observed at various distances (Z) from the axi...

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Figure 9: Left: TEM image of a Ag colloid prepared by laser ablation in acetone by femtosecond Bessel beams a...

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Figure 10: (a) A scheme of the experimental setup for nanostructuring with the nanosecond vortex beams. (b) Vo...

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Figure 11: Simulated intensity distributions. (a) Gaussian beam; (b) DS beam with the same pulse energy; (c) c...

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Figure 12: Time-resolved images of CBs in water produced by DS laser pulses at early evolution stages. (a) Las...

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Figure 13: Comparison of gold NPs produced by PLAL with picosecond radially-polarised DS and linearly polarise...

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Figure 14: (a) Experimental setup. Diffuser 1: holographic. Diffuser 2: glass diffuser or Scotch tape. Pulse e...

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Figure 15: Ag NPs colloidal solutions UV–vis spectra. Without irradiation (black), after 10 min (red), and 60 ...

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Figure 16: Comparison of pump–probe laser ablation experiments of gold immersed in air and water irradiated wi...

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Figure 17: (a) Schematic depiction of the pump–probe experimental setup. (b) Microscopy images of the time-res...

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Figure 18: (a) Normalised NP weight distribution as a function of the particle diameter for double-pulse delay...

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Figure 19: (a) Shadowgraph images of CBs produced by ps dual-beam PLAL of YAG in water at the energy in each p...

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Figure 20: Dependence of mass loss on the pulse duration for different pulse energy and 85 nm film thickness. Figure 20...

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Figure 21: Pulse width dependence with pulse energy for (a) ablated mass and (b) crater depth in water. (c) Cr...

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Figure 22: (a) Threshold fluence dependence on the pulse duration; insets: optical images of single-pulse crat...

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Figure 23: Images of Au colloids as function of the pulse energy (I – 100 µJ, II – 120 µJ, III – 140 µJ, IV – ...

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Figure 24: (a) Schematic illustration of the MB-PLAL process. (b) Productivity of FeNi NPs in water with a dif...

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Figure 25: Productivity of CrFeCoNiMn high entropy alloy NPs by ps PLAL in water with and without DOEs as a fu...

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Review

Published 16 Feb 2026

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