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Journal articles on the topic 'Laser Damage threshold'

Author: Grafiati

Published: 3 June 2025

Last updated: 31 July 2025

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1

Wilson, Steven E., and Richard F. Brubaker. "Neodymium:YAG Laser Damage Threshold." Ophthalmology 94, no. 1 (1987): 7–11. http://dx.doi.org/10.1016/s0161-6420(87)33500-6.

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2

Chen, Mingjun, Wenyu Ding, Jian Cheng, Hao Yang, and Qi Liu. "Recent Advances in Laser-Induced Surface Damage of KH2PO4 Crystal." Applied Sciences 10, no. 19 (2020): 6642. http://dx.doi.org/10.3390/app10196642.

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As a hard and brittle material, KDP crystal is easily damaged by the irradiation of laser in a laser-driven inertial confinement fusion device due to various factors, which will also affect the quality of subsequent incident laser. Thus, the mechanism of laser-induced damage is essentially helpful for increasing the laser-induced damage threshold and the value of optical crystal elements. The intrinsic damage mechanism of crystal materials under laser irradiation of different pulse duration is reviewed in detail. The process from the initiation to finalization of laser-induced damage has been

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3

Zhang, Luwei, Xiaodong Jia, Yunzhe Wang, et al. "Effect of Femtosecond Laser Polarization on the Damage Threshold of Ta2O5/SiO2 Film." Applied Sciences 12, no. 3 (2022): 1494. http://dx.doi.org/10.3390/app12031494.

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The study used linearly and circularly polarized femtosecond pulsed lasers to irradiate a Ta2O5/SiO2 film. Firstly, the damage thresholds of the film for linearly and circularly polarized femtosecond pulsed lasers were measured in 1-on-1 mode. The results showed that the damage threshold (1.70 J/cm2) under a circularly polarized laser was higher than that (1.68 J/cm2) under a linearly polarized laser. For femtosecond lasers, the multi-photon ionization cross-section under circular polarization was lower than that under linear polarization. The lower ionization rate under circular polarization

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4

Deng, Wenyuan, and Chunshui Jin. "Laser induced damage threshold testing of DUV optical substrates." Chinese Optics Letters 11, S1 (2013): S10702. http://dx.doi.org/10.3788/col201311.s10702.

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5

Chen, Qiao, He Wang, Rucheng Dai, et al. "Correlation between Photoluminescence Properties of Surface Defects and Laser-Induced Damage Threshold of Fused Silica." Laser and Particle Beams 2021 (June 22, 2021): 1–6. http://dx.doi.org/10.1155/2021/5530410.

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Laser-induced damage threshold is the main limitation for fused silica optics in high-power laser applications. The existence of various defects near the surface is the key factor for the degradation of the threshold. In this work, the photoluminescence spectra at different regions of the damaged and recovered fused silica samples are recorded to analyze the correlation between photoluminescence of surface defects and laser-induced damage threshold. The experimental data concluded the inverse proportional correlation between fluorescence and laser-induced damage threshold value. The weak photo

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6

Ahmed, Fakhruddin. "Laser damage threshold of KTiOPO_4." Applied Optics 28, no. 1 (1989): 119. http://dx.doi.org/10.1364/ao.28.000119.

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7

Nikolaeva, I. N., D. S. Gusev, L. S. Parshina, et al. "Damage threshold determination of MoS2 and NiO thin films by femtosecond laser pulses." Himičeskaâ fizika i mezoskopiâ 27, no. 1 (2025): 75–86. https://doi.org/10.62669/17270227.2025.1.8.

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This paper considers the interaction of femtosecond laser pulses with thin MoS2 and NiO films synthesized by pulsed laser deposition. The effect of the thin film thickness on the laser-damage threshold was investigated. The damage thresholds were experimentally determined for multiple irradiation with 128 fs laser pulses at a repetition rate of 1 kHz. The thresholds were found to be 33 and 15 mJ/cm2 for MoS2 films with a thickness of 20 and 29 nm; for NiO films with a thickness of 40, 85 and 170 nm the damage thresholds were 88, 97 and 54.9 mJ/cm2, respectively. Based on the two-temperature mo

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8

Bisson, Jean-François, Yang Feng, Akira Shirakawa, et al. "Laser Damage Threshold of Ceramic YAG." Japanese Journal of Applied Physics 42, Part 2, No. 8B (2003): L1025—L1027. http://dx.doi.org/10.1143/jjap.42.l1025.

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9

Wang, Jiamin, Kuo Zhang, Yanhui Ji, et al. "Damage Characteristics of Aluminum-Coated Grating Irradiated by Nanosecond Pulsed Laser." Coatings 12, no. 5 (2022): 701. http://dx.doi.org/10.3390/coatings12050701.

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An aluminum-coated grating (ACG) is a core component of laser systems and spectrometers. Understanding damage to the ACG induced by nanosecond lasers is critical for future high-power laser applications. In this study, we applied finite element simulation and practical experimentation to investigate the characteristics of ACG damage. Based on a coupling model using fluid heat transfer with the level-set method, we simulated the damage caused to an ACG by a 1064 nm nanosecond single pulse laser. The theoretical modeling showed that the ridge and bottom corners of the grid will be preferentially

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10

Xiaofeng Liu, 刘晓凤, 李大伟 Dawei Li, 赵元安 Yuan’an Zhao, 李笑 Xiao Li, 凌秀兰 Xiulan Ling, and 邵建达 Jianda Shao. "Automated damage diagnostic system for laser damage threshold tests." Chinese Optics Letters 8, no. 4 (2010): 407–10. http://dx.doi.org/10.3788/col20100804.0407.

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11

Yang, Liu, Liu Lisheng, Tang Wei, et al. "Experimental Study on the Damage of Optical Materials by out of Band Composite Laser." Applied Sciences 10, no. 10 (2020): 3578. http://dx.doi.org/10.3390/app10103578.

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For the paper, experimental studies were performed on the damage of the Ge- and Si-based flat window by lasers out-of-band. The experimental results showed that lasers out-of-band can cause film damage and substrate damage to Ge and Si windows. The high-energy laser damage window mechanism mainly manifested as thermal effects. The composite laser damage thresholds for the substrate were an Si window of 21.6 J/cm2 and a Ge window of 3 J/cm2. Compared with continuous laser and long pulse laser experimental results, it was found that the use of long pulse-continuous composite constitution could e

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12

Cui, Wen-Wen, Xiao-Wei Xing, Yue-Jia Xiao, and Wen-Jun Liu. "Research progress of mode-locked pulsed fiber lasers with high damage threshold saturable absorber." Acta Physica Sinica 71, no. 2 (2022): 024206. http://dx.doi.org/10.7498/aps.71.20212442.

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As the basic hardware to promote the development of various fields, fiber laser has great development potential in rail transit, optical communication, new material manufacturing, power battery processing, military defense, medical treatment, and other fields. As the core device of passively mode-locked fiber laser, a high damage threshold saturable absorber plays a decisive role in achieving high power, ultrashort pulse duration, and high energy laser output for a fiber laser. For saturable absorbers of traditional materials and structures, the spot size of light acting on the material is alm

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13

Du, Xiaoli, Zeliang Gao, Lijuan Chen, Youxuan Sun, and Xutang Tao. "High laser damage threshold LiNa5Mo9O30 prism: for visible to mid-infrared range." Chinese Optics Letters 20, no. 5 (2022): 051602. http://dx.doi.org/10.3788/col202220.051602.

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14

Gerhard, Christoph, and Marco Stappenbeck. "Impact of the Polishing Suspension Concentration on Laser Damage of Classically Manufactured and Plasma Post-Processed Zinc Crown Glass Surfaces." Applied Sciences 8, no. 9 (2018): 1556. http://dx.doi.org/10.3390/app8091556.

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The laser-induced damage threshold of optics is an issue of essential importance in high-power laser applications. However, the complex and partially interacting mechanisms as well as the underlying reasons for laser damage of glass surfaces are not yet fully understood. The aim of the present work is to contribute to a better understanding of such damage mechanisms by providing original results on the impact of classical glass surface machining on the laser-induced damage threshold. For this purpose, glass samples were prepared with well-defined process conditions in terms of the used lapping

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15

Tüzün, Pervin, Ömer Faruk Kadı, Fikret Yıldız, Ramiz Hamid, and Humbat Nasibov. "A Laser Damage Threshold for Microscope Glass Slides." Photonics 10, no. 9 (2023): 967. http://dx.doi.org/10.3390/photonics10090967.

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Laser-based light sources have fostered innovative developments in biomedical and biosensor fields. However, laser-induced damage to optical components is a limitation for designing and implementing highly sensitive biosensors, necessitating the development and characterization of suitable optical components. Microscope glass slides are among the most extensively used optical units in this field. This study investigated the laser-induced damage threshold (LIDT) of high-quality microscope glass slides obtained from three different vendors. An S-on-1 protocol following the ISO 21254 series stand

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16

Yudin, Nikolai, Oleg Antipov, Ilya Eranov, et al. "Laser-Induced Damage Threshold of Single Crystal ZnGeP2 at 2.1 µm: The Effect of Crystal Lattice Quality at Various Pulse Widths and Repetition Rates." Crystals 12, no. 5 (2022): 652. http://dx.doi.org/10.3390/cryst12050652.

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The ZnGeP2 crystal is a material of choice for powerful mid-IR optical parametric oscillators and amplifiers. In this paper, we present the experimental analysis of the optical damage threshold of ZnGeP2 nonlinear crystals induced by a repetitively-pulsed Ho3+:YAG laser at 2091 nm. Two types of ZnGeP2 crystals grown under different conditions were examined using the laser and holographic techniques. The laser-induced damage threshold (LIDT) determined by the pulse fluence or peak intensity was studied as a function of the pulse repetition rate (PRR) and laser exposure duration. The main crysta

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17

Edziah, Raymond. "High Repetition-Rate Laser Z-Scan Measurements: Criterion for Recognizing Adverse Thermal Effects." Applied Physics Research 11, no. 2 (2019): 73. http://dx.doi.org/10.5539/apr.v11n2p73.

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This study reports z-scan measurements in which high-repetition-rate and reduced repetition-rate (pulse-picked) laser beams were employed using a standard sample, carbon disulfide (CS2) contained in supposedly high damage-threshold spectroscopic-grade pristine fused-quartz cuvettes. The results suggest that at reduced repetition rates, the closed aperture z-scan profile for CS2 displays the expected configuration. However, at high repetition-rates the closed aperture z-scans are distinctly different resulting in unexpectedly large nonlinear refractive index of CS2 due to thermal effects that r

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18

Ding, Yi, Jun Hong Su, and Hai Feng Liang. "Acoustic Method of Detection of Optical Thin Films Damage." Advanced Materials Research 301-303 (July 2011): 965–69. http://dx.doi.org/10.4028/www.scientific.net/amr.301-303.965.

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Laser damage threshold of optical thin film is a critical parameter in measuring laser induced damage. The key to testing damage threshold is judging the injury incident accurately. It has been found that when high-energy laser on the film, there will be sounds generated. In the present paper, acoustic method was applied to determine thin films damage. A brief analysis will be given on feasibility of acoustic method in judging thin films damage. Acoustic acquisition system will be established. In the experiment, we will average laser energy into 10 grades, each grade test 10 points. The sound

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19

Li, Chao Yang, and Yong Gang Wang. "The Study of Femto-Second Laser Induced Damage Threshold on Semi-Insulating GaAs Wafer." Advanced Materials Research 31 (November 2007): 65–67. http://dx.doi.org/10.4028/www.scientific.net/amr.31.65.

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We demonstrated an experiment of femtosecond-laser damage threshold on GaAs wafer, the damage threshold was measured from 50 to 400fs. The mechanism was discussed through injection power, pulse duration and ablation profile. The results showed that the damage threshold increased with the pulse duration, the relationship between diameter of ablation hole and laser power density was also analyzed. It was concluded that the main factor affecting the damage threshold was photon ionization and collision ionization.

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20

Cech, Pavel, Jan Vanda, Mihaj-George Muresan, Martin Mydlar, Katerina Pilna, and Jan Brajer. "LASER INDUCED DAMAGE THRESHOLD TESTING AT HILASE." MM Science Journal 2019, no. 05 (2019): 3657–61. http://dx.doi.org/10.17973/mmsj.2019_12_2019118.

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21

Sakalauskas, Leonidas, and Ingrida Vaičiulytė. "Statistical modeling for laser induced damage threshold." Computational Science and Techniques 8 (October 4, 2021): 625–30. http://dx.doi.org/10.15181/csat.v8.2102.

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22

MIKAMI, Katsuhiro, Shinji MOTOKOSHI, Masayuki FUJITA, Takahisa JITSUNO, Junji KAWANAKA, and Ryo YASUHARA. "Laser-Induced Damage Threshold in Silica Glasses." Review of Laser Engineering 38, no. 6 (2010): 458–61. http://dx.doi.org/10.2184/lsj.38.458.

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23

Hu, Jianping, Jian Wang, Zhou Xin, Songlin Chen, Ma Ping, and Xu Qiao. "Fluence uncertainties of laser damage threshold measurements." Laser Physics 24, no. 1 (2013): 016003. http://dx.doi.org/10.1088/1054-660x/24/1/016003.

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24

Alvisi, M., M. Di Giulio, S. G. Marrone, et al. "HfO2 films with high laser damage threshold." Thin Solid Films 358, no. 1-2 (2000): 250–58. http://dx.doi.org/10.1016/s0040-6090(99)00690-2.

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25

Yudin, Nikolai Nikolayevich, Mikhail Zinoviev, Vladislav Gladkiy, et al. "Influence of the Characteristics of Multilayer Interference Antireflection Coatings Based on Nb, Si, and Al Oxides on the Laser-Induced Damage Threshold of ZnGeP2 Single Crystal." Crystals 11, no. 12 (2021): 1549. http://dx.doi.org/10.3390/cryst11121549.

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In this work, the effect of the defect structure and the parameters of antireflection interference coatings based on alternating layers of Nb2O5/Al2O3 and Nb2O5/SiO2 layers on the laser-induced damage threshold of ZGP crystals under the action of Ho:YAG laser radiation at a wavelength of 2.097 μm was determined. Coating deposition was carried out using the ion-beam sputtering method. The laser-induced damage threshold of the sample with a coating based on alternating layers Nb2O5 and SiO2 was W0d = 1.8 J/cm2. The laser-induced damage threshold of the coated sample based on alternating layers o

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26

Sun, Yuan Yuan, Li Zheng, Li Min Song, Qiu Rui Jia, and Shi Bo Liu. "Research on the Thermal Effect of Long Pulse Laser Irradiation BK7 Glass." Applied Mechanics and Materials 347-350 (August 2013): 1123–26. http://dx.doi.org/10.4028/www.scientific.net/amm.347-350.1123.

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The temperature and thermal stress distribution on BK7 glass was numerical simulated by MATLAB according to heat conduction theory. Research has shown that the laser pulse number, spot radius and pulse width can change the extent of the damage threshold for BK7 glass. The results shown the damage threshold decreased with the laser pulse number and radius increasing. The laser power also increased with the pulse width reducing. At the same time, the damage threshold was corresponding reduced.

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27

Zhang, Yin, Changbin Zheng, Yang Liu, Yunzhe Wang, Yongbo Xu, and Junfeng Shao. "Damage Mechanism of HgCdTe Focal Plane Array Detector Irradiated Using Mid-Infrared Pulse Laser." Sensors 23, no. 23 (2023): 9370. http://dx.doi.org/10.3390/s23239370.

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To investigate the damage threshold and mechanism of a mid-infrared HgCdTe focal plane array (FPA) detector, relevant experimental and theoretical studies were conducted. The line damage threshold of a HgCdTe FPA detector may be within the range of 0.59 Jcm−2 to 0.71 Jcm−2. The full frame damage threshold of the detector may be in the range of 0.86 Jcm−2 to 1.17 Jcm−2. Experimental results showed that when the energy density reaches 1.17 Jcm−2, the detector exhibits irreversible full frame damage and is completely unable to image. Based on the finite element method, a three-dimensional model o

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28

Varlamov, Pavel, Jan Marx, Yoav Urbina Elgueta, et al. "Femtosecond Laser Ablation and Delamination of Functional Magnetic Multilayers at the Nanoscale." Nanomaterials 14, no. 18 (2024): 1488. http://dx.doi.org/10.3390/nano14181488.

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Laser nanostructuring of thin films with ultrashort laser pulses is widely used for nanofabrication across various fields. A crucial parameter for optimizing and understanding the processes underlying laser processing is the absorbed laser fluence, which is essential for all damage phenomena such as melting, ablation, spallation, and delamination. While threshold fluences have been extensively studied for single compound thin films, advancements in ultrafast acoustics, magneto-acoustics, and acousto-magneto-plasmonics necessitate understanding the laser nanofabrication processes for functional

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29

DUAN, L. H., A. P. LIU, S. L. CHEN, et al. "RELATIONSHIP BETWEEN MICRO-STRUCTURE AND LASER DAMAGE THRESHOLD OF NANO-ZrO2 FILMS." International Journal of Modern Physics B 19, no. 01n03 (2005): 585–87. http://dx.doi.org/10.1142/s0217979205029092.

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In this paper, the micro-structure and laser damage threshold of nano- ZrO 2 thin films were investigated. High-purity nano- ZrO 2 particles as the coating materials of samples were prepared by the electron beams evaporation. The micro-structure and crystallitic size of samples were analyzed by X-ray diffraction, a laser by 1064nm, 10ns, 3Hz Nd:YAG laser damage test each for nano- ZrO 2 films. The results showed that oxygen partial pressure has an important influence on the micro-structure of nano- ZrO 2 films, also found that the crystallitic size and different micro-structure influenced the

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30

LENZNER, M. "FEMTOSECOND LASER-INDUCED DAMAGE OF DIELECTRICS." International Journal of Modern Physics B 13, no. 13 (1999): 1559–78. http://dx.doi.org/10.1142/s0217979299001570.

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Optical damage in non-metals (dielectrics) may severely affect the performance of high-power laser systems as well as the efficiency of optical systems based on nonlinear processes and has therefore been subject to extensive research for some 30 years. The current knowledge of laser-induced optical damage in these materials is reviewed. Emphasis is placed on the recent extension of available experimental data into the femtosecond range. Recent results are presented achieved with a sub-10 fs laser system which explores the limits of time resolution as well as the limit of intensities that a sol

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31

Narayanasamy, Priyadarshani, Martin Mydlář, Hana Turčičová, et al. "Investigation of UV Picosecond Laser Damage Threshold of Anti-Reflection Coated Windows." Journal of Manufacturing and Materials Processing 9, no. 6 (2025): 180. https://doi.org/10.3390/jmmp9060180.

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Long-term stability and laser-induced damage resistance of optical components in the UV region are critical for enhancing their performance in UV high-power laser applications. This study evaluates the laser-induced damage threshold (LIDT) of commercially available UV optical windows with anti-reflective (AR) coating, produced through various coating techniques and designed for high-power lasers. A third-harmonic (343 nm)wavelength with good beam quality was generated in the picosecond regime to investigate the LIDT of optical components. The LIDT for each sample was m

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32

Wang, Yunzhe, Xiangzheng Cheng, Junfeng Shao, Changbin Zheng, Anmin Chen, and Luwei Zhang. "The Damage Threshold of Multilayer Film Induced by Femtosecond and Picosecond Laser Pulses." Coatings 12, no. 2 (2022): 251. http://dx.doi.org/10.3390/coatings12020251.

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Laser-induced damage threshold (LIDT) is an essential factor in measuring the anti-laser damage of optical films. The damage threshold and morphology of the Ta2O5/SiO2 multilayer film prepared by electron beam evaporation were studied by femtosecond (50 fs) and picosecond (30 ps) laser irradiations. The results showed that the LIDT of the film was 1.7 J·cm−2 under the femtosecond laser. The damage morphology developed from surface damage to a clear layered structure, and the outline has become more transparent and regular with an increase in the laser fluence. Under the picosecond laser irradi

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33

Kerr, N. C., and D. C. Emmony. "The Effect of Laser Annealing on Laser-induced Damage Threshold." Journal of Modern Optics 37, no. 4 (1990): 787–802. http://dx.doi.org/10.1080/09500349014550851.

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34

Xia, Zhi Lin. "Experimental Investigation on Laser Pretreatment of Optical Films." Advanced Materials Research 189-193 (February 2011): 3713–16. http://dx.doi.org/10.4028/www.scientific.net/amr.189-193.3713.

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Optical films have been prepared on K9 glass by electronic beam evaporation. Parameters of S-polarized Nd: YAG laser used for pretreatment and damage tests are: wavelength is 355nm, pulse width is 8ns, and incidence angle is 33.75 degree. The results reflect that: the influence of laser pretreatment on laser induced damage threshold of films is uncertain. Laser pretreatment not always improve the laser induced damage threshold of films, and sometimes it will cause negative influence. As for damage probability, for a certain testing energy density, there is an energy density scope, pretreatment

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35

Junjiang Hu, Junjiang Hu, Lei Zhang Lei Zhang, Wei Chen Wei Chen, Changhe Zhou Changhe Zhou, and Lili Hu Lili Hu. "Experimental investigation on laser-induced surface damage threshold of Nd-doped phosphate glass." Chinese Optics Letters 10, no. 4 (2012): 041403–41406. http://dx.doi.org/10.3788/col201210.041403.

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36

Stevanovic, Igor, Zoltán Balogh-Michels, Andreas Bächli, et al. "Influence of the Secondary Ion Beam Source on the Laser Damage Mechanism and Stress Evolution of IBS Hafnia Layers." Applied Sciences 11, no. 1 (2020): 189. http://dx.doi.org/10.3390/app11010189.

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Ion beam sputtered hafnia is a preferred high index coating material for laser applications. It exhibits a mostly amorphous structure and an adequate laser-induced damage (LIDT) threshold. In this work, we investigated the influence of an assisting ion source on the film stress as well as the LIDT of the sputtered hafnia layers. The stress increases with an increasing ion energy of the assisting ion beam. We identified a maximum compressive stress of 3–3.5 GPa before the film cracks, blisters, and delaminates. Different states of stress lead to different laser-induced damage thresholds and dam

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37

Zhang, Ke, and Jingya Sun. "The dominant mechanism of gold film damage induced by near-threshold femtosecond laser: non-thermal deformation or thermal ablation." Journal of Physics: Conference Series 2313, no. 1 (2022): 012025. http://dx.doi.org/10.1088/1742-6596/2313/1/012025.

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Abstract Near-threshold femtosecond laser produces nanostructures on the gold film, which has received much attention in applications. However, the theoretical researches on the early stage of gold film excitation induced by the femtosecond laser are scarce, because of the ultrafast and non-equilibrium characteristics. In this study, stress and temperature distributions in different thicknesses of gold film induced by the near-threshold fluences were calculated. At the fluence below the melting threshold, we found that only the 30 nm gold films might be damaged by the non-thermal deformation.

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38

Liu, Le, Chengyang Xu, Sheng Cai, et al. "Research on the Damage Characteristics of a UAV Flight Control System Irradiated by a Continuous Laser." Aerospace 12, no. 2 (2025): 161. https://doi.org/10.3390/aerospace12020161.

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To improve laser anti-UAV technology and UAV laser protection capabilities, research on continuous laser damage to a UAV flight control system has been carried out. Combining waveform and function monitoring, the performance of the flight control system under laser irradiation was observed in real time, and the temperature and ablation process were recorded, which were used to analyze its damage characteristics and thresholds. Our experimental results show that the flight control system had two damage modes: temporary failure and permanent damage. Temporary failure had a temperature threshold,

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39

Li, Yuan, Junqi Xu, Guoliang Yang, Lihong Yang, and Junhong Su. "Quantifying Uncertainty in Laser-Induced Damage Threshold for Cylindrical Gratings." Micromachines 16, no. 1 (2024): 45. https://doi.org/10.3390/mi16010045.

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The laser-induced damage threshold (LIDT) is a key measure of an optical component’s resistance to laser damage, making its accurate determination crucial. Following the ISO 21254 standards, we studied the measurement strategy and uncertainty fitting method for laser damage, establishing a calculation model for uncertainty. Research indicates that precise LIDT measurement can be achieved by using a small energy level difference and conducting multiple measurements. The LIDT values for the cylindrical grating are 15.34 ± 0.00052 J/cm2 (95% confidence) and 15.34 ± 0.00078 J/cm2 (99% confidence),

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40

Wei, T. X., Z. Zhang, Z. Yang, Y. Sheng, and R. P. Wang. "Optical damage and the third-order nonlinearity in GeGaS glasses." Chalcogenide Letters 19, no. 9 (2022): 627–35. http://dx.doi.org/10.15251/cl.2022.199.627.

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We have measured optical properties of GexGa4S96-x (x=22.5, 27, 30, 33.3 and 36) glasses including optical bandgap Eg, hardness, linear and nonlinear refractive index and laser damage threshold. We found that, both Eg and laser damage threshold exhibit maximum values in Ge30Ga4S66 glass, linear refractive index increases with increasing Ge content, but nonlinear refractive index has a minimum in Ge30Ga4S66, and their correlation can be well described by the Miller’s rule. We conclude that, Ge30Ga4S66 glass with chemically stoichiometric composition might be ideal for the chalcogenide-based opt

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41

Trinavarat, Adisak, La-ongsri Atchaneeyasakul, and Suthipol Udompunturak. "Neodymium:YAG laser damage threshold of foldable intraocular lenses." Journal of Cataract & Refractive Surgery 27, no. 5 (2001): 775–80. http://dx.doi.org/10.1016/s0886-3350(00)00855-5.

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42

Venkataramanan, V., G. Dhanaraj, B. R. Prasad, C. K. Subramanian, and H. L. Bhat. "Laser damage threshold studies inL-Arginine Phosphate Monohydrate." Ferroelectrics 155, no. 1 (1994): 13–18. http://dx.doi.org/10.1080/00150199408007476.

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43

Thomas, Ian M. "High laser damage threshold porous silica antireflective coating." Applied Optics 25, no. 9 (1986): 1481. http://dx.doi.org/10.1364/ao.25.001481.

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44

Montgomery, Ken E., and Fred P. Milanovich. "High‐laser‐damage‐threshold potassium dihydrogen phosphate crystals." Journal of Applied Physics 68, no. 8 (1990): 3979–82. http://dx.doi.org/10.1063/1.346259.

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Li, Wei, Fangyuan Zha, Bo Fu, Yanglong Li, Jiazhu Duan, and Ziyou Zhou. "A Study on the Surface Quality and Damage Properties of Single-Crystal Silicon Using Different Post-Treatment Processes." Micromachines 15, no. 1 (2024): 145. http://dx.doi.org/10.3390/mi15010145.

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Detecting subsurface defects in optical components has always been challenging. This study utilizes laser scattering and photothermal weak absorption techniques to detect surface and subsurface nano-damage precursors of single-crystal silicon components. Based on laser scattering and photothermal weak absorption techniques, we successfully establish the relationship between damage precursors and laser damage resistance. The photothermal absorption level is used as an important parameter to measure the damage resistance threshold of optical elements. Single-crystal silicon elements are processe

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Batavičiutė, Gintarė, Povilas Grigas, Linas Smalakys, and Andrius Melninkaitis. "Revision of laser-induced damage threshold evaluation from damage probability data." Review of Scientific Instruments 84, no. 4 (2013): 045108. http://dx.doi.org/10.1063/1.4801955.

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Liu, Wenfeng, Mingying Sun, Yajing Guo, et al. "Effect of Dual-Pulse Temporal Shaping on Ultraviolet Nanosecond Laser Damage of Fused Silica Surface in High Fluence Regime." Photonics 9, no. 11 (2022): 834. http://dx.doi.org/10.3390/photonics9110834.

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We present the effect of dual-pulse temporal shaping on the ultraviolet nanosecond laser damage characteristics of a fused silica exit surface in a high fluence regime. The pre- and post-pulse have the opposite effects on the damage behavior at a pulse delay of 20 ns. The pre-pulse irradiation significantly increases the main-pulse threshold, making it much higher than that of the single-pulse threshold, while the post-pulse has little effect on the main-pulse threshold. For near-threshold damage sites, the pre-pulse reduces the average damage size and depth, making them smaller than those of

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Zou, Feng, Jun Qi Xun, Jun Hong Su, and Jian Bo Ma. "Influence of Laser-Conditioning on Laser-Induced Damage Properties of ZnSe Thin Films." Advanced Materials Research 602-604 (December 2012): 1437–43. http://dx.doi.org/10.4028/www.scientific.net/amr.602-604.1437.

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With the development of high power laser systems, laser protection of optical components becomes more and more important. In order to enhance the laser-induced damage capability of optical films components, besides advanced methods and processes, post-treatment has significant influence on the laser-induced damage threshold (LIDT) of thin films. Q switch Nd:YAG laser of the working wave length at 1064nm, was used to post process on ZnSe single layer films with thickness of /2 (=1064nm) deposited by thermal evaporation, and the laser-induced damage and optical properties were investigated. By

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Zhang, Yuhui, Yanzhi Wang, Hongbo He, et al. "Effect of Electric Field Regulation on Laser Damage of Composite Low-Dispersion Mirrors." Coatings 11, no. 1 (2021): 65. http://dx.doi.org/10.3390/coatings11010065.

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Low dispersion mirrors are important because of their potential use in petawatt (PW) laser systems. The following two methods are known to increase the laser-induced damage threshold of low dispersion optical components: use of a wide-bandgap-material protective layer and control of electric field distribution. By controlling the electric field distribution of composite low-dispersion mirrors (CLDM), we shift the electric field peaks from the material interface into the wide-bandgap material. However, the damage threshold of modified-electric-field composite low dispersion mirror (E-CLDM) does

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Zhang, Yuhui, Yanzhi Wang, Hongbo He, et al. "Effect of Electric Field Regulation on Laser Damage of Composite Low-Dispersion Mirrors." Coatings 11, no. 1 (2021): 65. http://dx.doi.org/10.3390/coatings11010065.

Full text

Abstract:

Low dispersion mirrors are important because of their potential use in petawatt (PW) laser systems. The following two methods are known to increase the laser-induced damage threshold of low dispersion optical components: use of a wide-bandgap-material protective layer and control of electric field distribution. By controlling the electric field distribution of composite low-dispersion mirrors (CLDM), we shift the electric field peaks from the material interface into the wide-bandgap material. However, the damage threshold of modified-electric-field composite low dispersion mirror (E-CLDM) does

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