2014
DOI: 10.1070/qe2014v044n06abeh015448
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Ablation and nanostructuring of metals by femtosecond laser pulses

Abstract: Using an interferometric continuous monitoring technique, we have investigated the motion of the surface of an aluminium target in the case of femtosecond laser ablation at picosecond time delays relative to the instant of laser exposure. Measurements of the temporal target dispersion dynamics, molecular dynamics simulation results and the morphology of the ablation crater have demonstrated a thermomechanical (spall) nature of the disruption of the condensed phase due to the cavitation-driven formation and gro… Show more

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Cited by 40 publications
(8 citation statements)
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“…The latter is most probably the consequence of a laser-induced nucleation or spallation process at fluences around the melting threshold, process that exhibits a statistical dependence of an Arhenius-like activation energy. A first laser pulse interacting with an initially flat surface close to ablation threshold nucleates solid-liquid transitions 17 , 33 at specific “weak” sites, triggering subsurface voids formation, swelling or hydrodynamic instabilities 34 . This randomly modifies the topography of the surface seen by a second pulse, for which the light coupling will be more complex.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…The latter is most probably the consequence of a laser-induced nucleation or spallation process at fluences around the melting threshold, process that exhibits a statistical dependence of an Arhenius-like activation energy. A first laser pulse interacting with an initially flat surface close to ablation threshold nucleates solid-liquid transitions 17 , 33 at specific “weak” sites, triggering subsurface voids formation, swelling or hydrodynamic instabilities 34 . This randomly modifies the topography of the surface seen by a second pulse, for which the light coupling will be more complex.…”
Section: Resultsmentioning
confidence: 99%
“…The ultimate size of the modification is then defined mainly by the material response to energy absorption and transport, with scales significantly smaller than those related to light confinement. This response can be of thermomechanical, hydrodynamic, or ablative nature 1 , 17 , 18 . One of the most spectacular laser nanostructuring processes is the formation of sub-wavelength ripples on materials ranging from metals to dielectrics.…”
Section: Introductionmentioning
confidence: 99%
“…Thermocapillary and Marangoni effects as well as Rayleigh–Plateau instability have been identified to influence the structure formation and its disintegration process [ 23 , 24 ]. Later on, however, the relaxation of the laser-induced stresses, generated in the vicinity of the target’s surface as a result of the laser heating, has been determined as a main driving mechanism responsible for the nanostructures growth [ 25 , 26 , 27 ]. The specifics of the final nanostructures shape depend on the material as well as on the laser parameters, the dynamical changes of the reflectivity of the material [ 28 , 29 ], and the geometric parameters of the irradiation pattern.…”
Section: Introductionmentioning
confidence: 99%
“…The steps are approximately homogeneous temperature distributions inside the liquid layers, while the intervals between the steps are the rather steep rises of temperature in a vapor layer between two neighboring liquid layers. In real 3D geometry the foamy zone contains a mixture of membranes, droplets, and vapor [1,39,40,41]. Vapor surrounding the droplets is weakly conductive.…”
Section: Separation Of Acoustic Zones and Hot Advection Layermentioning
confidence: 99%