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Lasers Technology | Progress Report  37





               can be created by ultrashort laser pulses (,)   parameters were used to investigate the influ-
               and in this case the modifications induced by   ence of metals electron mobility and thermal
               a pulse modify the Fth value for the following   conductivity on the ablation dynamics, the
               pulses, until the defects density reaches sat-  glasses ablation mechanism dependence on
               uration and Fth stabilizes at a constant value.   the pulse duration, and to texturize mechani-
               These cumulative phenomena are known as        cal tools to improve their performance and re-
               incubation effects, and the ablation threshold   duce wear, and to promote selective ablation.
               fluency modifications caused by them must
               be considered when machining a material. A     An interferometric system to maintain the la-
               few years ago(,) we introduced a simple ex-    ser focal point on the surface of a material be-
               perimental technique, denominated D-Scan       ing processed is under development. This sys-
               (Diagonal Scan), to quickly measure the ultra-  tem is based on the ultrashort pulses large
               short pulses ablation threshold of a solid sam-  bandwidth, and will improve the quality of
               ple. Recently(,) we modified this technique to   the machining.
               allow the ablation threshold measurement
               for an arbitrary pulse superposition (,) and   During the ablation by ultrashort pulses, the
               the consequently determination of the incu-    explosive material removal creates shockwaves
               bation effects. Knowing the ablation thresh-   that propagate into the substrate under irra-
               old for the superposition of multiple pulses is   diation. These shockwaves, besides promoting
               important when machining samples with ul-      a local increase in the pressure, also rise the
               trashort pulses, in which the sample displace-  temperature in a propagating submicron lay-
               ment speed and laser repetition rate play an   er. These conditions can be extreme and highly
               important role in setting the pulses overlap,   localized(,) due to the violent explosion result-
               and determine the morphology and quality       ing from the ultrashort pulses high intensity,
               of the structures etched. Our technique pres-  and promote modifications in the substrate.
               ents advantages over the traditional one due   We have demonstrated that the ablation origi-
               to its speed and for also (for) reproducing the   nated shockwaves in amorphous graphite can
               machining conditions more closely. Using the   change the hybridization of the carbon bonds
               results obtained for the superposition of many   from sp2 to sp3, increasing the order of the
               pulses, new methods were developed to etch     crystalline array, cumulatively creating dif-
               structures in the surfaces of technological ma-  ferent allotropes including nanodiamonds.
               terials minimizing the material modifications   Figure 1a shows  a High Resolution Electron
               on the neighborhood of the etched regions.     Diffraction of the diamond-like phase, and
                                                              Fig. 1b shows the same analysis  of the initial
               Using the D-Scan, we have determined the ab-   polycrystalline graphite (PG) substrate; Fig. 1c
               lation threshold of many materials, including   presents a  High Resolution Electron Microg-
               glasses, metals, graphite and ceramics, among   raphy of the laser created structure with the
               others. The ablation threshold dependence on   characteristic 0.205 nm d-spacing of the dia-
               the pulses superposition is an important pa-   mond phase evidenced by the zoom of a small
               rameter when machining these materials to      area shown in the bottom inset. Fig. 1d exhib-
               create microstructures such as microfluidic and   its the corresponding electron diffraction peaks
               microoptofluidic (micro opto-fluidic) circuits   as a function of the inverse of the d-spacing
               that are being developed and built at the Cen-  for the polycrystalline graphite (PG, gray spec-
               ter for Lasers and Applications at IPEN. These   trum) and diamond-like phase (blue spectrum).
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