Laser damage of UV hafnia-based multilayer dielectric coatings at 355  nm wavelength

Megajoule ultraviolet nanosecond pulses were used to demonstrate ignition at the National Ignition Facility in December 2022 [Nature601, 542 (2022)10.1038/s41586-021-04281-w]. The energy scaling of laser fusion drivers relies, in part, on significant improvements in the UV multilayer dielectric (MLD) coatings, which are critical optics in the laser architecture. This paper reports on the laser damage behavior of MLD coatings based on <i>H</i><i>f</i><i>O</i><sub>2</sub>, <i>S</i><i>i</i><i>O</i><sub>2</sub>, and <i>A</i><i>l</i><sub>2</sub><i>O</i><sub>3</sub>, designed for operation at <i>λ</i>=355<i>n</i><i>m</i>. Two-layer anti-reflection (AR) coatings containing <i>H</i><i>f</i><i>O</i><sub>2</sub>-based mixtures were co-sputtered by reactive biased target deposition (BTD) as the high-index layer. The laser-induced damage threshold was assessed from 1-on-1 and S-on-1 tests and compared to MLD ARs of <i>H</i><i>f</i><i>O</i><sub>2</sub>/<i>S</i><i>i</i><i>O</i><sub>2</sub> fabricated by ion beam sputtering and electron beam evaporation. It is shown that the 1-on-1 LIDT of BTD ARs, which contain <i>H</i><i>f</i><sub>1-<i>y</i></sub><i>S</i><i>i</i><sub><i>y</i></sub><i>O</i><sub><i>x</i></sub> and <i>H</i><i>f</i><sub>1-<i>y</i></sub><i>A</i><i>l</i><sub><i>y</i></sub><i>O</i><sub><i>x</i></sub> mixtures, is higher than that of BTD <i>H</i><i>f</i><i>O</i><sub>2</sub>/<i>S</i><i>i</i><i>O</i><sub>2</sub> ARs. However, this increase is below that predicted by the scaling of LIDT with the optical bandgap, calculated from the LIDT of <i>H</i><i>f</i><i>O</i><sub>2</sub>/<i>S</i><i>i</i><i>O</i><sub>2</sub> and <i>H</i><i>f</i><i>O</i><sub>2</sub>/<i>A</i><i>l</i><sub>2</sub><i>O</i><sub>3</sub>. The S-on-1 LIDT of BTD ARs decreases by ∼25<i>%</i> for <i>S</i>=10 and remains unchanged to <i>S</i>=10<sup>4</sup> laser shots, indicating no accumulation fatigue. Neither UV preconditioning nor etching of the substrate prior to coating deposition caused a major improvement in the 1-on-1 LIDT of BTD ARs.

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Publication Details

Journal
Applied Optics
Published
2025-02-26
DOI
https://doi.org/10.1364/ao.557518
Citations
2
Primary Topic
Laser Material Processing Techniques
Type
article
Field-Weighted Citation Impact
2.67
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article

Laser damage of UV hafnia-based multilayer dielectric coatings at 355  nm wavelength

Carmen S. Menoni, Maxwell Weiss, M. Chicoine, F. Schiettekatte et al.
2 citations
Applied Optics
Laser Material Processing Techniques
2.67
article

Laser damage of UV hafnia-based multilayer dielectric coatings at 355  nm wavelength

Carmen S. Menoni, Maxwell Weiss, M. Chicoine, F. Schiettekatte, Walter Siehien
article en
2 citations

Abstract

Megajoule ultraviolet nanosecond pulses were used to demonstrate ignition at the National Ignition Facility in December 2022 [Nature601, 542 (2022)10.1038/s41586-021-04281-w]. The energy scaling of laser fusion drivers relies, in part, on significant improvements in the UV multilayer dielectric (MLD) coatings, which are critical optics in the laser architecture. This paper reports on the laser damage behavior of MLD coatings based on <i>H</i><i>f</i><i>O</i><sub>2</sub>, <i>S</i><i>i</i><i>O</i><sub>2</sub>, and <i>A</i><i>l</i><sub>2</sub><i>O</i><sub>3</sub>, designed for operation at <i>λ</i>=355<i>n</i><i>m</i>. Two-layer anti-reflection (AR) coatings containing <i>H</i><i>f</i><i>O</i><sub>2</sub>-based mixtures were co-sputtered by reactive biased target deposition (BTD) as the high-index layer. The laser-induced damage threshold was assessed from 1-on-1 and S-on-1 tests and compared to MLD ARs of <i>H</i><i>f</i><i>O</i><sub>2</sub>/<i>S</i><i>i</i><i>O</i><sub>2</sub> fabricated by ion beam sputtering and electron beam evaporation. It is shown that the 1-on-1 LIDT of BTD ARs, which contain <i>H</i><i>f</i><sub>1-<i>y</i></sub><i>S</i><i>i</i><sub><i>y</i></sub><i>O</i><sub><i>x</i></sub> and <i>H</i><i>f</i><sub>1-<i>y</i></sub><i>A</i><i>l</i><sub><i>y</i></sub><i>O</i><sub><i>x</i></sub> mixtures, is higher than that of BTD <i>H</i><i>f</i><i>O</i><sub>2</sub>/<i>S</i><i>i</i><i>O</i><sub>2</sub> ARs. However, this increase is below that predicted by the scaling of LIDT with the optical bandgap, calculated from the LIDT of <i>H</i><i>f</i><i>O</i><sub>2</sub>/<i>S</i><i>i</i><i>O</i><sub>2</sub> and <i>H</i><i>f</i><i>O</i><sub>2</sub>/<i>A</i><i>l</i><sub>2</sub><i>O</i><sub>3</sub>. The S-on-1 LIDT of BTD ARs decreases by ∼25<i>%</i> for <i>S</i>=10 and remains unchanged to <i>S</i>=10<sup>4</sup> laser shots, indicating no accumulation fatigue. Neither UV preconditioning nor etching of the substrate prior to coating deposition caused a major improvement in the 1-on-1 LIDT of BTD ARs.

Applied OpticsVol. 64(11)
Vilnius University (LT), XUV Lasers (United States) (US), Blue Ridge Physical Therapy (US), Laboratoire d'Informatique en Images et Systèmes d'Information (FR), Université de Montréal (CA), Colorado State University (US)
Openalex Percentile: Top 14%
Laser Material Processing Techniques
2.67
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