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Picosecond-pulsed laser ablation of aluminum foils: crater morphology and plasma parameters

Munisbek AkhmedovDepartment of Technique, Urgench State University, Kh. Alimjan Str. 14, Urgench 220100, UzbekistanJurabek SadullayevDepartment of Technique, Urgench State University, Kh. Alimjan Str. 14, Urgench 220100, UzbekistanMurodbek VapayevDepartment of Technique, Urgench State University, Kh. Alimjan Str. 14, Urgench 220100, UzbekistanA. MatnazarovUrgench Innovation University, st. Town Independence MFY, 2nd House, Urgench, 220100, UzbekistanI.Yu. DavletovDepartment of Technique, Urgench State University, Kh. Alimjan Str. 14, Urgench 220100, UzbekistanJavlon RayimbaevNational University of Uzbekistan, Tashkent 100174, Uzbekistan
ABI

Аннотация

Abstract In this study, the ablation process that occurs on the surface of aluminum foil (Al) using picosecond-duration Nd: YAG laser pulses ( λ = 1064 nm, τ = 28 ps) and the physical properties of the resulting laser-induced plasma are comprehensively investigated. In the performed experiments, we used laser fluences ranging from 16.37 to 21.17 J cm −2 . The shape and dimensions of the craters formed on the surface are precisely analyzed using a Scanning Electron Microscope (SEM). Additionally, the spectral emission of the plasma is also examined using optical emission spectroscopy. The experimental results revealed a strong linear correlation between the diameter of the crater and the plasma electron density (R = 0.96). Our findings suggest the potential of laser-induced breakdown spectroscopy (LIBS) technology for improved precision and the development of minimally destructive surface analysis approaches. The plasma temperature is determined based on the Boltzmann distribution and found to have a direct dependence on the laser fluence. An increase in laser intensity resulted in a corresponding increase in the hydrodynamic length of the plasma. Furthermore, the inverse Bremsstrahlung absorption coefficient, which accounts for energy absorption in the plasma, is calculated, and its dependence on the laser fluence is confirmed with a high level of statistical confidence (R 2 = 0.99556).

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