### Abstract

Original language | English |
---|---|

Pages (from-to) | 1325-1333 |

Journal | Physics procedia |

Volume | 56 |

DOIs | |

Publication status | Published - 2014 |

### Fingerprint

### Keywords

- IR-91724
- METIS-304990

### Cite this

*Physics procedia*,

*56*, 1325-1333. https://doi.org/10.1016/j.phpro.2014.08.058

}

*Physics procedia*, vol. 56, pp. 1325-1333. https://doi.org/10.1016/j.phpro.2014.08.058

**Finite-difference Time-domain Modeling of Laser-induced Periodic Surface Structures.** / Römer, Gerardus Richardus, Bernardus, Engelina; Skolski, J.Z.P.; Vincenc Obona, J.; Huis in 't Veld, Bert.

Research output: Contribution to journal › Article › Academic › peer-review

TY - JOUR

T1 - Finite-difference Time-domain Modeling of Laser-induced Periodic Surface Structures

AU - Römer, Gerardus Richardus, Bernardus, Engelina

AU - Skolski, J.Z.P.

AU - Vincenc Obona, J.

AU - Huis in 't Veld, Bert

N1 - Open access. 8th International Conference on Laser Assisted Net Shape Engineering LANE 2014, Peer-review under responsibility of the Bayerisches Laserzentrum GmbH

PY - 2014

Y1 - 2014

N2 - 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 LIPSSs. 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 LIPSSs 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

AB - 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 LIPSSs. 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 LIPSSs 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

KW - IR-91724

KW - METIS-304990

U2 - 10.1016/j.phpro.2014.08.058

DO - 10.1016/j.phpro.2014.08.058

M3 - Article

VL - 56

SP - 1325

EP - 1333

JO - Physics procedia

JF - Physics procedia

SN - 1875-3892

ER -