MECHANISM OF DYE-ENHANCED PULSED-LASER ABLATION OF HARD TISSUES - IMPLICATIONS FOR DENTISTRY

Alexandrite laser ablation of enamel enhanced by indocyanine green dye was studied, Microjet system was employed to deliver precisely measur ed small amounts of absorbing dye solution to the site of irradiation, A sequence of physical phenomena involved in dye-enhanced laser ablat ion of dental enamel was revealed when laser pulse profiles were compa red with the profiles of laser-induced pressure, laser-induced plasma, and ablation plume kinetics, To understand photomechanical effects on the enamel ablation, the absolute values of pressure waves were measu red by calibrated wide-band acoustic transducer. Absolute amplitude an d temporal profile of pressure waves, plasma emission, ablation plume kinetics, ablation efficiency, and crater quality under free-running a nd Q-switched ablation of enamel were studied, It was found that there is an optimal dye solution volume (100-200 nL) when the maximum ablat ion efficiency (30 mu m/pulse) can be obtained, It was shown that the ablation efficiency under Q-sn;itched laser irradiation is approximate ly one order of magnitude lower than that under free-running ablation, It was shown that Q-switched enamel ablation with dye solution is cau sed by the powerful recoil pressure wave with the amplitude 3-6.5 kbar , In contrast, dye-enhanced free-running enamel ablation is caused by plasma-mediated evaporation of enamel and accompanied by recoil pressu re waves of lower amplitude (0.5-1 kbar) that is below mechanical dama ge threshold in enamel. Uneven crater walls after Q-switched ablation were observed by scanning electron microscopy (SEM), Free-running abla tion makes precise craters with smooth and even crater walls.