Elsevier

Applied Surface Science

Volume 186, Issues 1–4, 28 January 2002, Pages 352-357
Applied Surface Science

Modification of dielectric surfaces with ultra-short laser pulses

https://doi.org/10.1016/S0169-4332(01)00675-4Get rights and content

Abstract

Crater morphology is investigated after femtosecond laser ablation of wide bandgap insulators (BaF2 and CaF2). Experiments performed at a weak laser ablation rate show a particular elastic, sound wave-like structure, frozen on the surface, with a periodicity in the order of some microns and a modulation depth up to 0.5 μm. When superimposed, a periodic fine structure (ripples) is generated, the origin of which cannot be explained in the classical ripple model. We observe a periodicity ranging from 100 to 500 nm, dependent on the laser intensity rather than on the laser wavelength. Based on our recent results, demonstrating an explosive surface decomposition, we assume self-organizing relaxation of a non-equilibrium surface to be responsible for the structures.

Introduction

Surface damage ablation with ultra short, sub-picosecond laser pulses has been investigated for intentional high-precision material processing [1], [2], and for the study of the dynamics in laser materials interaction [3], [4]. Considering laser ablation from transparent wide bandgap dielectrics, these investigations [5], [6], [7] have confirmed the mechanism previously proposed [8], [9], [10] that multiphoton surface ionization is followed by Coulomb explosion of positive ions from an electrostatically unstable surface. The competing model of surface super-heating resulting in phase explosion [11] does not seem to play an important role in this case, being considered to correspond only to strong absorption, e.g. in metals, semiconductors or at much higher intensities in insulators [12].

In this contribution, we demonstrate that the morphology of the irradiated surfaces yields valuable details concerning the microscopic mechanisms involved in laser ablation, in particular, femtosecond laser ablation.

For instance, it is well known that the periodic structures occur on the bottom of the sub picosecond ablated crater [13], [14]. They look very similar to those observed previously on various metals, semiconductors, and insulators upon irradiation ranging from CW to nanosecond pulses. In a classical model [15], these structures correspond to a non-uniform energy input into the sample, modulated by the interference between the incident wave and an induced (evanescent) surface wave.

Section snippets

Experiments

Our experiments were carried out on freshly cleaved single crystal slides of BaF2 and CaF2, under high vacuum (<10−7 mbar) and irradiated with ultra-short laser pulses provided by an amplified Ti:sapphire laser system, with 800 nm central wavelength and 1 kHz repetition rate. Pulse duration was 120 fs and pulse energy <0.5 mJ. Experiments were performed using p-polarized and s-polarized beams focused on the target by using single spherical quartz lenses (f=+300and+500mm). Additionally,

Results

We examined the ablated craters produced on BaF2 (also in CaF2) by ultra-short laser pulses with intensities of 1–12×1012W/cm2, applying several thousand laser pulses per spot (1000–10 000). At these intensities, the ablation rate was rather moderate, i.e. of about 5 nm/pulse at 0.8×1013W/cm2, as determined using white light interference microscopy.

We note that the crater morphology particularities observed in BaF2 were relatively equivalent in CaF2. Therefore, we proceed to expose our results

Discussion

From our previous studies [5], [6], we know that positive ions are emitted explosively with mean kinetic energies in the order of 100 eV. However, the energy distribution corresponds only to a surface temperature of 1 eV (104 K), a typical value for plasma. As the origin for this difference between kinetic energy and temperature, Coulomb explosion after strong surface ionization was invoked. This means, that the laser input results first in an electrostatically highly unstable surface and then the

Acknowledgements

We would like to thank Prof. Dr. D. Linke for the opportunity to use his high resolution optical microscope, and W. Seifert, S. Pandelov, and T. Arguirov for their support with the electron microscopy.

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