scholarly journals Femtosecond laser-induced damage threshold of nematic liquid crystals at 1030  nm

2021 ◽  
Vol 60 (26) ◽  
pp. 8050
Author(s):  
Loic Ramousse ◽  
Gilles Chériaux ◽  
Cyrille Claudet ◽  
Aurélie Jullien
2021 ◽  
Author(s):  
Loïc Ramousse ◽  
Gilles Chériaux ◽  
Cyrille Claudet ◽  
Aurélie Jullien

2015 ◽  
Vol 117 (22) ◽  
pp. 223103 ◽  
Author(s):  
L. Gallais ◽  
D.-B. Douti ◽  
M. Commandré ◽  
G. Batavičiūtė ◽  
E. Pupka ◽  
...  

2019 ◽  
Author(s):  
Agnė Butkutė ◽  
Linas Jonušauskas ◽  
Darius Gailevičius ◽  
Vygantas Mizeikis ◽  
Mangirdas Malinauskas

2014 ◽  
Vol 5 ◽  
pp. 1334-1340 ◽  
Author(s):  
Wataru Nomura ◽  
Tadashi Kawazoe ◽  
Takashi Yatsui ◽  
Makoto Naruse ◽  
Motoichi Ohtsu

The laser-induced damage threshold (LIDT) is widely used as an index for evaluating an optical component’s resistance to laser light. However, a degradation in the performance of an optical component is also caused by continuous irradiation with laser light having an energy density below the LIDT. Therefore, here we focused on the degradation in performance of an optical component caused by continuous irradiation with femtosecond laser light having a low energy density, i.e., laser-induced degradation. We performed an in situ observation and analysis of an increase in scattering light intensity in fused silica substrates. In experiments conducted using a pulsed laser with a wavelength of 800 nm, a pulse width of 160 fs and pulse repetition rate of 1 kHz, we found that the scattered light intensity increased starting from a specific accumulated fluence, namely, that the laser-induced degradation had a threshold. We evaluated the threshold fluence F t as 6.27 J/cm2 and 9.21 J/cm2 for the fused silica substrates with surface roughnesses of 0.20 nm and 0.13 nm in R a value, respectively, showing that the threshold decreased as the surface roughness increased. In addition, we found that the reflected light spectrum changed as degradation proceeded. We analyzed the details of the degradation by measuring instantaneous reflectance changes with a pump–probe method; we observed an increase in the generation probability of photogenerated carriers in a degraded silica substrate and a damaged silica substrate and observed a Raman signal originating from a specific molecular structure of silica. From these findings, we concluded that compositional changes in the molecular structure occurred during degradation due to femtosecond laser irradiation having an energy density below the LIDT.


2016 ◽  
Vol 56 (1) ◽  
pp. 011001 ◽  
Author(s):  
Adrien Hervy ◽  
Laurent Gallais ◽  
Gilles Chériaux ◽  
Daniel Mouricaud

2017 ◽  
Vol 636 ◽  
pp. 289-295 ◽  
Author(s):  
Hossein Shahrokhabadi ◽  
Majid Vaezzadeh ◽  
Alireza Bananej ◽  
Mohamad Hadi Maleki

2008 ◽  
Author(s):  
N. Sanner ◽  
B. Bussiere ◽  
O. Utéza ◽  
A. Leray ◽  
T. Itina ◽  
...  

Coatings ◽  
2020 ◽  
Vol 10 (6) ◽  
pp. 603 ◽  
Author(s):  
Praveen Kumar Velpula ◽  
Daniel Kramer ◽  
Bedrich Rus

The laser-induced damage threshold (LIDT) of optical components is one of the major constraints in developing high-power ultrafast laser systems. Multi-layer dielectric (MLD) coatings-based optical components are key parts of high-power laser systems because of their high damage resistance. Therefore, understanding and characterizing the laser-induced damage of MLD coatings are of paramount importance for developing ultrahigh-intensity laser systems. In this article, we overview the possible femtosecond laser damage mechanisms through damage morphologies in various MLD optical coatings tested in our facility. To evaluate the major contributions to the coating failure, different LIDT test methods (R-on-1, ISO S-on-1 and Raster Scan) were carried out for a high reflective hybrid Ta2O5/HfO2/SiO2 MLD mirror coating at a pulse duration of 37 fs. Different LIDT test methods were compared due to the fact that each test method exposes the different underlying damage mechanisms. For instance, the ISO S-on-1 test at a higher number of laser pulses can bring out the fatigue effects, whereas the Raster Scan method can reveal the non-uniform defect clusters in the optical coating. The measured LIDT values on the sample surface for the tested coating in three test methods are 1.1 J/cm2 (R-on-1), 0.9 J/cm2 (100k-on-1) and 0.6 J/cm2 (Raster Scan) at an angle of incidence of 45 deg. The presented results reveal that the performance of the tested sample is limited by coating defects rather than fatigue effects. Hence, the Raster Scan method is found to be most accurate for the tested coating in evaluating the damage threshold for practical applications. Importantly, this study demonstrates that the testing of different LIDT test protocols is necessary in femtosecond regime to assess the key mechanisms to the coating failure.


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