Acta Optica Sinica, Volume. 44, Issue 17, 1732015(2024)

Progress on Ultrafast Laser Coatings with Ultrabroadband High‐Threshold and Dispersion Modulation (Invited)

Jianda Shao1,2,3、*, Lin Jia1,4, Chang Liu1,2, Tianze Xu1,2, Yu Chen1、**, and Yanzhi Wang1、***
Author Affiliations
  • 1Laboratory of Thin Film Optics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2College of Materials Science and Opto-Electronic Technology, University of Chinese Academy of Sciences, Beijing 100049, China
  • 3Hangzhou Institute for Advanced Study, University of Chinese Academy of Sciences, Hangzhou 310024, Zhejiang , China
  • 4School of Physical Science and Technology, ShanghaiTech University, Shanghai 201210, China
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    Figures & Tables(36)
    Sculptured chirp mirror[35]. (a) Structural schematic, substrate, chirped film stack, and low-index layer, from bottom to top;(b) schematic refractive index profile of the chirp mirror
    Structure of wedged dispersive mirror[36]
    GDD curves of complementary paired dispersive mirrors, the red and blue curves represent the GDD of the CM 1 and CM 2 dispersive mirrors, respectively, and the green curve represents the GDD of the paired mirrors[37]
    Double angle dispersion mirror[38]. (a) Conceptual diagram of double-angle dispersive mirror; (b) GDD pairing curves of double-angle dispersive mirror
    Non-uniformity paired dispersive mirror[40]. (a)(b) GD and GDD of pair of complementary paired dispersive mirrors prepared with non-uniformity; (c) thickness of the dispersive mirror film layer is adjusted by setting the mirrors at different positions of the preparation disc
    Reflectivity and time delay for broadband mirrors, high-threshold mirrors and optimised broadband high-threshold mirrors[42]
    Laser-induced damage threshold of different highly reflective mirrors measured at 1030 nm with a 350 ps pulse[43]
    Broadband low-dispersion mirror coatings structure[47]. (a) Schematic diagram of low-dispersion mirror based on quarter-wavelength layer structure; (b) chirped reflector with increased layer thickness demonstrating negative GDD; (c) schematic diagram of new low-dispersion mirror based on top periodically chirped layer and bottom structured quarter-wavelength layer
    Low dispersion mirror with hump structure[15]. (a) Schematic diagram of broadband reflector based on sinusoidal modulation structure; (b) schematic diagram of new low-dispersion mirror based on hump and QWOT structures; (c)(d) reflectivity and dispersion of QWOT structure, hump structure and whole structure
    Schematic diagram of common deposition techniques. (a) Schematic diagram of magnetron sputtering[52]; (b) schematic diagram of ion beam sputtering[53]
    Schematic diagram of oblique angle deposition[54]
    Structural schematic of a high laser damage threshold reflective thin film system[56]. (a) Schematic of conventional combined film system design using alternating structures of high and low refractive index materials; (b) schematic of the design of new nano-stacked membrane system using alternating structures of nano-stacked and low refractive index materials
    Opto-mechanical design of the in situ broadband monitoring, incoming optical system (left) and outgoing optical system (right)[57]
    Schematic diagram of in-situ phase measurement monitoring system[58]
    Schematic diagram of on-line measurement system for spectral phase information[59]
    Schematic diagram of real-time interference monitoring system[61]
    Principle diagram of white light interferometer[53]
    Reversibility of the nonlinear response of the dispersive mirror, with error bars representing the measurement error[74]
    Pump-probe experimental results. (a) Temperature rise under the irradiation of a 30 fs pulse and a 1 ps pulse[75]; (b) optical path diagram of the pump-probe experiment[76]; (c) evolution of normalized reflectivity over time at different wavelengths[76]
    Compression results of dispersive mirror[78]. (a) TiO2/SiO2 dispersive mirror; (b) HfO2/SiO2 dispersive mirror
    Electric field distribution with different numbers of protective layers[82]. (a) Electric field of the combined low-dispersive mirror with different numbers of protective layers, as the number of Al2O3 layers increases, the electric field in the narrow bandgap material decreases; (b) electric field of the optimized combined low-dispersive mirror with different numbers of protective layers
    Schematic diagram of peak electric field intensity[84]. (a) Design with peak electric field intensity located within high-index layers; (b) field-optimized design with peak electric field intensity located within low-index layers
    High damage threshold dispersion mirror with low equivalent electric field[87].(a) Film structure of dispersive mirror with high threshold; (b) distribution of electric field intensity with wavelength; (c) distribution of electric field intensity at 790 nm and 810 nm, as well as the average value within the first 4 μm of the film layers; (d) distribution of equivalent electric field intensity; (e) normalized spectrum of the incident pulse
    Time-domain dynamic electric field model[88]. (a) Time-domain electric field distribution atwavelength of 800 nm; (b) time-domain electric field distribution at multiple wavelengths; (c) time-domain electric field distribution through Bragg mirror at multiple wavelengths; (d) local time-domain electric field intensity at the surface of 1 μm
    Laser induced damage characteristics of chirped mirrors. (a) Evolution of blister morphology on a dispersive mirror with varying incident pulse energy[86]; (b) evolution of blister morphology on a highly dispersive mirror with varying incident pulse energy[90]
    History of laser peak power[95]. (a) Development of peak power, key technologies and facilities; (b) chirped pulse amplification mechanism
    SULF prototype laser[95]
    Domestic and foreign representative products of broadband high damage threshold low dispersion ultrafast laser coatings. (a) Laseroptik GmbH, German; (b) Sandia National Laboratories, USA; (c) Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, China
    Interferometric autocorrelation function of the measured pulse using a prepared double-angle dispersive mirror, indicating a pulse duration of 4.3 fs[38]
    Schematic diagram of the optical path structure of fully chirped mirror compensated Ti∶Sapphire laser[97]
    Pulse compression experiment results[98]. (a) Experimental D-scan traces of few-cycle pulses; (b) measured spectra (blue curve) and retrieved spectral phases (red curve); (c) temporal intensity envelope of Fourier transform limited pulse (blue curve) and retrieved pulses (red curve)
    Principle diagram of post-compression technique[101]
    Post-compression technique[102]. (a) Principle diagram of post-compression; (b) experimental demonstration of five-fold pulse compression and broadened spectrum in single-stage fused silica thin plate compressor; (c) results from two-stage fused silica thin plate compressor
    Schematic layout of the Er fiber chirped pulse amplification with the high-dispersion mirror compressor[16]
    Experimental normalized electric field in time domain, duration of chirped pulse intensity full width at half maximum is 86 fs, compressed pulse duration is 55 fs[108]
    Measured results of Cr∶ZnS laser system for different configurations[110]
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    Jianda Shao, Lin Jia, Chang Liu, Tianze Xu, Yu Chen, Yanzhi Wang. Progress on Ultrafast Laser Coatings with Ultrabroadband High‐Threshold and Dispersion Modulation (Invited)[J]. Acta Optica Sinica, 2024, 44(17): 1732015

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    Paper Information

    Category: Ultrafast Optics

    Received: Jun. 7, 2024

    Accepted: Jul. 8, 2024

    Published Online: Sep. 9, 2024

    The Author Email: Shao Jianda (jdshao@siom.ac.cn), Chen Yu (chenyu4@siom.ac.cn), Wang Yanzhi (yanzhiwang@siom.ac.cn)

    DOI:10.3788/AOS241152

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