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1.
Rev Sci Instrum ; 94(12)2023 Dec 01.
Article in English | MEDLINE | ID: mdl-38059764

ABSTRACT

The knowledge of the laser damage resistance of fused silica optics for their use in high-power lasers is of primary importance for the operation and maintenance of these facilities. Among the control procedures developed, one of the most relevant to date is the raster scan procedure [Lamaignère et al., Rev. Sci. Instrum. 78, 103105 (2007)]. This procedure is used to determine the damage density of optical components as a function of fluence. To date, this procedure takes into account all triggered damage sites, regardless of their size and/or morphology. We have added a step to this procedure, which consists in irradiating again all the damage sites with a series of shots to ascertain their ability to grow. This allows us to estimate the densities of growing damage sites, which are most critical for the safe operation of lasers. This pragmatic approach can be considered a functional test procedure. By applying this procedure to large optical areas, we were then able to measure extremely low damage densities (∼10-4 damage cm-2) over a wide range of fluences [0-18 J cm-2], corresponding to fluences to which the optics are irradiated during the operation of high-power lasers. We can then determine the damage law of a given set of optical components. This reference law makes it possible, on the one hand, to predict the lifetime of the optics. On the other hand, any deviation can then be analyzed with regard to this reference law. Thanks to the determination of confidence intervals, this functional procedure can also be used to delimit the reference law by upper and lower bounds.

2.
Appl Opt ; 59(32): 10061-10068, 2020 Nov 10.
Article in English | MEDLINE | ID: mdl-33175780

ABSTRACT

High-power nanosecond laser pulses are usually spectrally broadened via temporal phase modulations to tackle the issue of stimulated Brillouin scattering and to achieve optical smoothing of the focal spot. While propagating along the beamline, such pulses can undergo frequency modulation to amplitude modulation (FM-to-AM) conversion. This phenomenon induces modulations of the optical power that can have a strong impact on laser performance. Interference filters are specific FM-to-AM conversion contributors that lead to high-frequency modulations that cannot be measured using conventional means. We propose an indirect method to investigate for such FM-to-AM contributors using spectral measurements. Further analysis of the collected data makes the quantification of the defining parameters of interference filters possible. In turn, we show that it is possible to estimate the range of power modulations induced by interference filters.

3.
Rev Sci Instrum ; 90(7): 073001, 2019 Jul.
Article in English | MEDLINE | ID: mdl-31370447

ABSTRACT

We report on the implications that the temporal and spatial beam metrologies have on the accuracy of temporal scaling laws of Laser Induced Damage Threshold (LIDT) for dielectric materials in the picosecond regime. Thanks to a specific diagnostic able to measure the temporal pulse shape of subpicosecond and picosecond pulses, we highlight through simulations and experiments how the temporal shape has to be taken into account first in order to correctly understand the temporal dependency of dielectrics LIDT. This directly eases the interpretation of experimental temporal scaling laws of LIDT and improves their accuracy as a prediction means. We also give numerically determined benchmark temporal scaling laws of intrinsic LIDT for SiO2 (thin film) based on the model developed for this work. Finally, we show as well what kind of spatial metrology is needed during any temporal scaling law determination to take into account potential variations of the spatial profile.

4.
Opt Express ; 27(12): 16922-16934, 2019 Jun 10.
Article in English | MEDLINE | ID: mdl-31252910

ABSTRACT

Owing to their relatively high resistance to laser-induced damage, hafnia and silica are commonly used in multilayered optical coatings in high-power laser facilities as high- and low-refractive-index materials, respectively. Here, we quantify the laser-induced-damage threshold (LIDT) at 1053 nm in the short-pulse regime of hafnia and silica monolayers deposited by different fabrication methods, including electron-beam evaporation, plasma ion-assisted deposition and ion-assisted deposition. The results demonstrate that nominally identical coatings fabricated by different deposition techniques and/or vendors can exhibit significantly different damage thresholds. A correlation of the LIDT performance of each material with its corresponding absorption edge is investigated. Our analysis indicates a weak correlation between intrinsic LIDT and the optical gap of each material (Tauc gap) but a much better correlation when considering the spectral characteristics in the Urbach tail spectral range. Spectrophotometry and photothermal absorption were used to provide evidence of the correlation between the strength of the red-shifted absorption tail and reduced LIDT at 1053 nm.

5.
Rev Sci Instrum ; 90(12): 125102, 2019 Dec 01.
Article in English | MEDLINE | ID: mdl-31893816

ABSTRACT

The determination of the laser damage resistance of optics in the nanosecond regime is based on statistical tests and approaches because the response of the components is mainly related to the presence of defects randomly distributed in the optics and is therefore probabilistic in nature. For practical reasons, the tests are mostly carried out with beams of small dimensions (several tens of micrometer), that make it possible to determine a damage probability from which a laser damage threshold is extracted. This threshold is, however, highly correlated with the size of the test beam and the sampling of the test procedure. Some measurements are also made with beams of large dimensions (several millimeters) from which a damage density is determined. However, the relationship between the damage probability and the damage density is not trivial. It is based on assumptions that are difficult to verify because the experimental validations are carried out on different laser installations. In order to study accurately the coherence between these tests with small and large beams, as well as the link between damage probability and damage density, it is necessary to perform measurements on the same laser installation. We propose here, to compare for the first time, the results obtained with the same laser source with a large beam and also with small beams. The small beams are shaped from phase objects specifically implemented to obtain several small beams from a single larger beam. The consistency of the laser damage that results from both sets of measurements is demonstrated here. It validates the assumptions made and the specific mathematical treatment implemented to establish the link between the two approaches. In fine, it also validates and strengthens the approach previously developed from the rasterscan procedure [Lamaignère et al., Rev. Sci. Instrum. 78, 103105 (2007)] used to measure damage densities from the scanning of optics with beams of small dimensions. The reported original work based on phase objects thus makes it possible to replicate small beam tests with a large beam facility. The comparison between the results from the small beams and the results from the large beam experiments definitively makes the link between damage probabilities and damage densities. This also shows that small beam tests are reasonable representative of tests carried out with large beams.

6.
Opt Express ; 25(15): 16957-16970, 2017 Jul 24.
Article in English | MEDLINE | ID: mdl-28789195

ABSTRACT

The Petawatt Aquitaine Laser (PETAL) facility was designed and constructed by the French Commissariat à l'énergie atomique et aux énergies alternatives (CEA) as an additional PW beamline to the Laser MegaJoule (LMJ) facility. PETAL energy is limited to 1 kJ at the beginning due to the damage threshold of the final optics. In this paper, we present the commissioning of the PW PETAL beamline. The first kJ shots in the amplifier section with a large spectrum front end, the alignment of the synthetic aperture compression stage and the initial demonstration of the 1.15 PW @ 850 J operations in the compression stage are detailed. Issues encountered relating to damage to optics are also addressed.

7.
Opt Lett ; 41(14): 3237-40, 2016 Jul 15.
Article in English | MEDLINE | ID: mdl-27420504

ABSTRACT

Thanks to a phase-modulated injection seeder, we report the operation of a nanosecond Nd:YAG Q-switched laser with pulses having both a large spectral bandwidth and a smooth temporal waveform. Because of the smooth temporal waveform, such pulses allow, for instance, reducing the impact of the Kerr effect and, because of the large spectral bandwidth, suppressing stimulated Brillouin scattering. We conducted a parametric study of the features of the generated pulses versus the injection conditions. We show that, as opposed to the central frequency (wavelength) of the seeder, the phase modulation frequency has to be carefully chosen, but it is not a critical parameter and does not require any particular feedback.

8.
Opt Lett ; 39(3): 674-7, 2014 Feb 01.
Article in English | MEDLINE | ID: mdl-24487896

ABSTRACT

In our study, the laser-induced damage densities on a fused silica surface produced by multiple longitudinal mode (MLM) pulses are found to be higher than those produced by single longitudinal mode pulses at 1064 nm. This behavior is explained by the enhancement of the three-photon absorption due to the intensity spikes related to longitudinal mode beating. At 355 nm, the absorption is linear and an opposite behavior occurs. It can be explained with the help of a process involving thermomechanics coupled with the fine time structure of MLM pulses, leading to the possible annealing of part of the absorbent defects.

9.
Opt Express ; 21(23): 28272-89, 2013 Nov 18.
Article in English | MEDLINE | ID: mdl-24514338

ABSTRACT

We investigate the efficiency of local CO2laser processing of scratches on silica optics in order to enhance the nanosecond UV-laser damage resistance. The surface deformations induced by the process have been measured for different CO2laser parameters and then the pulse duration and the beam diameter have been chosen accordingly to limit those deformations below 1 µm. From the study of the laser damage resistance as a function of different material modifications we identify a range of optimal radiation parameters allowing a complete elimination of scratches associated with a high threshold of laser damage. Calculation of the temperature of silica using a two-dimensional axi-symmetric code was compared with experiment, supporting an optimization of the laser parameter as a function of the maximal dimensions of scratches that could be removed by this process.

10.
Opt Express ; 18(25): 26068-76, 2010 Dec 06.
Article in English | MEDLINE | ID: mdl-21164955

ABSTRACT

CO(2) laser is an interesting tool to repair defects on silica optics. We studied UV nanosecond laser-induced damage in fused silica after CO(2) laser heating. The localization of damage sites and the laser damage threshold are closely related to stress area in silica induced by heating. By applying a suitable second laser heating, we managed to eliminate the debris issued from redeposited silica and to modify the stress area. As a consequence, a significant increase of laser resistance has been observed. This process offers the possibility to improve damage repairing sufficiently to extend the lifetime of the silica components.


Subject(s)
Heating/instrumentation , Heating/methods , Lasers, Gas , Silicon Dioxide/chemistry , Silicon Dioxide/radiation effects , Welding/instrumentation , Welding/methods , Equipment Design , Equipment Failure Analysis
11.
Rev Sci Instrum ; 78(10): 103105, 2007 Oct.
Article in English | MEDLINE | ID: mdl-17979404

ABSTRACT

Known for more than 40 years, laser damage phenomena have not been measured reproducibly up to now. Laser resistance of optical components is decreased by the presence of material defects, the distribution of which can initiate a distribution of damage sites. A raster scan test procedure has been used for several years in order to determine laser damage density of large aperture UV fused silica optics. This procedure was improved in terms of accuracy and repeatability. We describe the equipment, test procedure, and data analysis to perform this damage test of large aperture optics with small beams. The originality of the refined procedure is that a shot to shot correlation is performed between the damage occurrence and the corresponding fluence by recording beam parameters of hundreds of thousands of shots during the test at 10 Hz. We characterize the distribution of damaging defects by the fluence at which they cause damage. Because tests are realized with small Gaussian beams (about 1 mm at 1e), beam overlap and beam shape are two key parameters which have to be taken into account in order to determine damage density. After complete data analysis and treatment, we reached a repeatable metrology of laser damage performance. The measurement is destructive for the sample. However, the consideration of error bars on defect distributions in a series of parts allows us to compare data with other installations. This will permit to look for reproducibility, a necessary condition in order to test theoretical predictions.


Subject(s)
Algorithms , Lasers , Materials Testing/instrumentation , Models, Theoretical , Silicon Dioxide/radiation effects , Computer Simulation , Data Interpretation, Statistical , Equipment Design , Equipment Failure Analysis , Materials Testing/methods , Reproducibility of Results , Sensitivity and Specificity
12.
Opt Express ; 13(25): 10163-71, 2005 Dec 12.
Article in English | MEDLINE | ID: mdl-19503232

ABSTRACT

In this paper we study the effect of contamination induced by fabrication process on laser damage density of fused silica polished parts at 351 nm in nanosecond regime. We show, owing to recent developments of our raster scan metrology, that a good correlation exists between damage density and concentration of certain contaminants for the considered parts.

13.
Phys Rev Lett ; 77(13): 2738-2741, 1996 Sep 23.
Article in English | MEDLINE | ID: mdl-10062033
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