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3 article(s) from Doñate-Buendia, Carlos

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

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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

Full text

Synthesis and magnetic transitions of rare-earth-free Fe–Mn–Ni–Si-based compositionally complex alloys at bulk and nanoscale

Shabbir Tahir,
Tatiana Smoliarova,
Carlos Doñate-Buendía,
Michael Farle,
Natalia Shkodich and
Bilal Gökce

Beilstein J. Nanotechnol. 2025, 16, 823–836, doi:10.3762/bjnano.16.62

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Figure 1: Synthesis route of the Ge- and Al-based CCAs. (a) Bulk Ge-based CCA produced via HEBM of elemental ...

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Figure 2: (a, c) SEM (SE) and EDX elemental maps of Mn, Fe, Ni, Ge, and Si obtained for bulk the Ge-based CCA...

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Figure 3: Particle size distribution extracted from TEM images (inset) from (a) bulk Ge-based CCA and (b) bul...

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Figure 4: (a) Mn, Fe, Ni, Ge, and Si EDX elemental maps of the PLAL-generated CCA NPs from the bulk Ge-based ...

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Figure 5: High-resolution TEM images and diffractograms of PLAL-generated CCA NPs. (a) Ge-based CCA NP and (b...

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Figure 6: (a) ZFC-FC temperature-dependent magnetization (M–T curve) of the bulk Ge-based CCA. (b) Field-depe...

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Figure 7: (a) ZFC-FC temperature-dependent magnetization (M–T) curves of NPs generated from PLAL of the Ge-ba...

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Full Research Paper

Published 05 Jun 2025

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Size control of nanoparticles synthesized by pulsed laser ablation in liquids using donut-shaped beams

Abdel Rahman Altakroury,
Oleksandr Gatsa,
Farbod Riahi,
Zongwen Fu,
Miroslava Flimelová,
Andrei Samokhvalov,
Stephan Barcikowski,
Carlos Doñate-Buendía,
Alexander V. Bulgakov and
Bilal Gökce

Beilstein J. Nanotechnol. 2025, 16, 407–417, doi:10.3762/bjnano.16.31

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Figure 1: (a) Schematic of the experimental setup for beam shaping and PLAL. (b, c) Intensity profiles of the...

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Figure 2: Comparison of gold NPs produced by PLAL with radially polarized donut-shaped and Gaussian laser bea...

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Figure 3: Comparison of Y₂O₃ NPs produced by PLAL with donut-shaped and Gaussian laser beams at a pulse energ...

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Figure 4: Comparison of HEA NPs produced by PLAL with Gaussian and donut-shaped laser beams at a pulse energy...

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Figure 5: Shadowgraph images of the cavitation bubbles produced by (a) Gaussian pulse and (b) donut-shaped pu...

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Full Research Paper

Published 25 Mar 2025

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