Finite-difference time-domain modeling of laser-induced periodic surface structures

被引:18
|
作者
Romer, G. R. B. E. [1 ]
Skolski, J. Z. P. [1 ,2 ]
Obona, J. Vincenc [1 ,2 ]
in 't Veld, A. J. Huis [1 ]
机构
[1] Univ Twente, Chair Appl Laser Technol, Drienerlolaan 5, NL-7522 NB Enschede, Netherlands
[2] M2i Mat Innovat Inst, NL-2628 CD Delft, Netherlands
关键词
Laser-induced Periodic Surface Structures; Model; LIPSS; Maxwell curl equations; FDTD; ABLATION; PULSES; METALS; DAMAGE; IRRADIATION; SPALLATION; TIN; SI;
D O I
10.1016/j.phpro.2014.08.058
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Laser-induced periodic surface structures (LIPSSs) consist of regular wavy surface structures with amplitudes the (sub)micrometer range and periodicities in the (sub)wavelength range. It is thought that periodically modulated absorbed laser energy is initiating the growth of LIPS S s. The "Sipe theory" (or "Efficacy factor theory") provides an analytical model of the interaction of laser radiation with a rough surface of the material, predicting modulated absorption just below the surface of the material. To address some limitations of this model, the finite-difference time-domain (FDTD) method was employed to numerically solve the two coupled Maxwell's curl equations, for linear, isotropic, dispersive materials with no magnetic losses. It was found that the numerical model predicts the periodicity and orientation of various types of LIPS Ss which might occur on the surface of the material sample. However, it should be noted that the numerical FDTD model predicts the signature or "fingerprints" of several types of LIPSSs, at different depths, based on the inhomogeneously absorbed laser energy at those depths. Whether these types of (combinations of) LIPSSs will actually form on a material will also depend on other physical phenomena, such as the excitation of the material, as well as thermal-mechanical phenomena, such as the state and transport of the material. (C) 2014 The Authors. Published by Elsevier B.V.
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页码:1325 / 1333
页数:9
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