Abstract:A study of the surface modification induced by single femtosecond laser pulses in phosphate glass has revealed surface swelling at fluences just below the ablation threshold. This behavior is different from that observed in other dielectric materials. Optical micrographs obtained with monochromatic light show a pattern of Newton rings within the swollen region whose number scales inversely with the illumination wavelength, acting as a micro Fabry-Perot etalon. The swollen surface layer has lower refractive ind… Show more
“…The nature of such rings was initially attributed to shockwaves in the surface due to hydrodynamic effects in the melted material [12]. Recent studies [14] have demonstrated that the melted material acts as a micro Fabry-Perot etalon formed between the laser-produced top layer of lower refractive index than the underneath bulk material, separated by a sharp optical interface. A study of the number, thickness and displacement of the dynamically moving Newton fringes allows the generation of different quantitative parameters as the thickness of the melted volume, the dynamic of the refractive index of the melted pool and the estimation of the electron plasma density [15].…”
“…The nature of such rings was initially attributed to shockwaves in the surface due to hydrodynamic effects in the melted material [12]. Recent studies [14] have demonstrated that the melted material acts as a micro Fabry-Perot etalon formed between the laser-produced top layer of lower refractive index than the underneath bulk material, separated by a sharp optical interface. A study of the number, thickness and displacement of the dynamically moving Newton fringes allows the generation of different quantitative parameters as the thickness of the melted volume, the dynamic of the refractive index of the melted pool and the estimation of the electron plasma density [15].…”
“…This fact indicates that the ratio between the number of fringes and wavelength is approximately constant, verifying the interferometric origin for the fringe pattern, corresponding to Newton fringes caused by a semitransparent, superficially modified surface layer. We previously observed and studied this kind of interference effect for irradiations in phosphate glass, using 100 fs transformlimited pulses [25]. In the current investigation, we modeled the ring pattern observation by analogy with a micro-FabryPerot system, a laser-induced thin surface layer with different optical properties as sketched in Fig.…”
Fused silica surface structuring has been performed using temporally shaped femtosecond laser pulses. For this purpose we have designed pulse bursts with a triangular intensity envelope and different slope sign and interpulse separation that were experimentally generated using a home-made temporal pulse shaper. We have found that pulse bursts with decreasing intensity envelopes are remarkably more efficient in terms of surface ablation than bursts with increasing intensity envelopes. The results reveal that laser energy coupling in the material is enhanced as the interpulse spacing decreases. A study of the ablation depth using stretched single pulses was carried out and compared to results obtained for pulse bursts with different interpulse spacing. We find that the deepest crater was achieved with bursts of 0.5 ps interpulse separation and decreasing envelope. This pulse form also induced the largest change of the surface reflectivity after irradiation. The results are discussed in terms of how the laser energy coupling efficiency is linked to the temporal pulse shape.
“…7 Second, it features surface swelling at fluences just below the ablation threshold (F th ¼ 3.8 J/cm 2 ), offering an ideal fluence window for studying the formation and evolution of the HAL without being shielded by ablation effects. 7,12 Figure 2 shows the effect induced by a single pulse at a fluence of 3.7 J/cm 2 , slightly below the ablation threshold. The optical microscopy (OM) image shows the appearance of Newton rings.…”
Section: -9mentioning
confidence: 99%
“…Using a simple Drude model, a maximum carrier density of n e ¼ 1.1 Â 10 22 cm À3 can be estimated. 12 At t ¼ 20 ps, the reflectivity has decreased below that of the non-excited material (by a factor $0.5). While this behavior might be interpreted as a sign of ablation, it should be kept in mind that the fluence employed is below the ablation threshold (see the AFM image in Fig.…”
Section: -9mentioning
confidence: 99%
“…6, which expresses T m as a function of depth and time assuming a value for A $ 0.5. Using a value for n e ¼ 1.1 Â 10 22 cm À3 , 12 we obtain 110 6 10 nm as the optical penetration depth. As material parameters, we have used T m ¼ 950 K (Ref.…”
Several studies in dielectrics have reported the presence of a thin heat-affected layer underneath the ablation crater produced by femtosecond laser irradiation. In this work, we present a time-resolved microscopy technique that is capable of monitoring the formation dynamics of this layer and apply it to the study of a phosphate glass exposed to single pulses below the ablation threshold. A few nanoseconds after laser excitation, a melt front interface can be detected, which propagates into the bulk, gradually slowing down its speed. By means of image analysis combined with optical modeling, we are able to determine the temporal evolution of the layer thickness and its refractive index. Initially, a strong transient decrease in the refractive index is observed, which partially recovers afterwards. The layer resolidifies after approximately 1 μs after excitation, featuring a maximum thickness of several hundreds of nanometers.
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