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Research on Thermal Effect and Laser-Induced Damage Threshold of 10.6 µm Antireflection Coatings Deposited on Diamond and ZnSe Substrates

MetadataDetails
Publication Date2025-04-30
JournalCoatings
AuthorsXiong Zi, Xinshang Niu, Hongfei Jiao, Shuai Jiao, Xiaochuan Ji
InstitutionsShanghai University, Tongji University
AnalysisFull AI Review Included

This study systematically investigated the performance of 10.6 µm Anti-Reflection (AR) coatings (ZnS/YbF3) deposited on Chemical Vapor Deposition (CVD) diamond versus standard Zinc Selenide (ZnSe) substrates under Continuous Wave (CW) laser irradiation.

  • Superior Thermal Management: The AR coating on the diamond substrate exhibited a 36% lower maximum temperature rise (62.5 °C vs. 96.63 °C) compared to the ZnSe substrate under identical 2830 W/cm2 CW laser irradiation.
  • Enhanced LIDT: The Laser-Induced Damage Threshold (LIDT) for the diamond-AR coating was 15,287 W/cm2, representing a 28.5% improvement over the ZnSe-AR coating (11,890 W/cm2).
  • Thermal Uniformity: Diamond’s exceptional thermal conductivity (2000 W/(m·K)) resulted in highly uniform temperature distribution, reducing the maximum lateral temperature gradient from 18.2 °C (ZnSe) to 0.1 °C (Diamond).
  • Spectral Performance: The 9-layer ZnS/YbF3 AR coating achieved excellent spectral properties, with transmission exceeding 98% at 10.6 µm on both substrates.
  • Damage Mechanism: Damage on ZnSe was characterized by melting, cracking, and perforation due to thermal runaway. Damage on diamond involved melting, localized graphitization (phase transition), fracture, and perforation.
  • Conclusion: CVD diamond is highly promising as an output window material for high-power 10.6 µm laser systems due to its superior thermal stability and higher LIDT, despite its slightly higher optical absorption coefficient compared to ZnSe.
ParameterValueUnitContext
Target Wavelength10.6µmCO2 Laser System
AR Coating StructureZnS/YbF3 (9 layers)N/ATotal thickness 1.5 µm
Transmission (Diamond-AR)98.04%At 10.6 µm
Transmission (ZnSe-AR)98.48%At 10.6 µm
Diamond Thermal Conductivity2000W/(m·K)Room Temperature
ZnSe Thermal Conductivity16W/(m·K)Room Temperature
Diamond LIDT (CW)15,287W/cm260 s irradiation time
ZnSe LIDT (CW)11,890W/cm260 s irradiation time
LIDT Improvement (Diamond)28.5%Relative to ZnSe substrate
Max Temp Rise (Diamond-AR)62.5°CUnder 2830 W/cm2 CW laser (200 s)
Max Temp Rise (ZnSe-AR)96.63°CUnder 2830 W/cm2 CW laser (200 s)
Temp Rise Reduction (Diamond)36%Relative to ZnSe substrate
Max Lateral Temp Gradient (Diamond)0.1°CSimulated result
Max Lateral Temp Gradient (ZnSe)18.2°CSimulated result
Diamond Extinction Coefficient (10.6 µm)2.61 x 10-6N/AOptical absorption
ZnSe Extinction Coefficient (10.6 µm)6.01 x 10-7N/AOptical absorption
Diamond Thermal Expansion1.1 x 10-6K-1Low stress generation
ZnSe Thermal Expansion7.1 x 10-6K-1High stress generation
RMS Surface Roughness (Diamond-AR)2.3nmAFM measurement
RMS Surface Roughness (ZnSe-AR)2.5nmAFM measurement

The 10.6 µm AR coatings were fabricated using a Leybold ARES 1110 vacuum deposition system, combining thermal evaporation and ion-assisted deposition (IAD).

  1. Substrate Preparation:

    • Substrates (Φ25.4 x 1 mm CVD diamond and ZnSe) were cleaned using an ion beam from an APS source prior to deposition to enhance adhesion.
    • Ion source parameters: Voltage 120 V, Current 40 mA.
  2. Film Deposition Parameters:

    • Vacuum pressure: 8 x 10-6 mbar.
    • Substrate temperature: Maintained at 150 °C (optimized to balance packing density and sulfur loss in ZnS).
    • ZnS Deposition: Thermal evaporation using a molybdenum boat. Rate: 1.0 nm/s.
    • YbF3 Deposition: Ion-assisted thermal evaporation (IAD used to reduce moisture absorption). Rate: 0.5 nm/s.
  3. Optical and Structural Characterization:

    • Transmittance: Measured using a Fourier-transform infrared spectrometer (INVENIOS, Bruker) at 0° incidence.
    • Surface Morphology: Investigated via Atomic Force Microscopy (AFM) (Bruker instrument) over a 2 µm x 2 µm area.
    • Crystallinity: Determined using X-ray diffraction (XRD) (Rigaku instrument, Cu Kα).
    • Microstructure: Cross-sectional SEM imaging (FIB-SEM, Cross Beam 350) after Au coating and focused ion beam sectioning.
  4. Thermal and Damage Testing (CW Laser):

    • Laser System: Custom CO2 laser system (Huazhong University of Science and Technology).
    • Beam Parameters: Gaussian beam, 1/e2 diameter 1.5 mm, M2 < 1.15.
    • Temperature Rise Test: Laser power 50 W (2830 W/cm2 density), irradiation time 200 s. Temperature monitored by a thermocouple (2 ± 0.5 mm from spot center).
    • LIDT Test: Laser power step size 10 W, irradiation time 60 s per step. Damage observed via Leica microscope and FIB-SEM.

The development of high-performance, thermally stable AR coatings on CVD diamond substrates is critical for advancing systems that rely on high-power 10.6 µm CO2 lasers.

  • High-Power Industrial Laser Processing: Used in cutting, welding, and surface modification where high beam quality and stable output power are essential. Diamond windows minimize thermal lensing distortion, ensuring precise beam focus.
  • Directed Energy Systems (Defense/Aerospace): Output windows for high-energy laser weapons require materials with extreme thermal shock resistance and high LIDT to maintain operational stability under intense CW irradiation.
  • Laser Dielectric Acceleration: Components requiring high-power transmission windows in advanced particle accelerator research.
  • Extreme Ultraviolet (EUV) Lithography: While the paper focuses on 10.6 µm, diamond’s broad transparency and thermal properties make it suitable for managing heat loads in complex optical trains used in EUV generation and delivery systems.
  • High-Power Optical Components: Fabrication of robust beamsplitters, mirrors, and lenses where thermal stability prevents catastrophic failure and wavefront degradation.
View Original Abstract

In this study, ZnS/YbF3-10.6 µm antireflection (AR) coatings were fabricated on CVD single-crystal diamond and ZnSe substrates. The spectral characteristics of the coatings and their performance under continuous wave laser radiation at 10.6 µm were systematically investigated. The fabricated AR coatings exhibited excellent spectral properties in the target wavelength range. Both theoretical calculations and experimental results indicated that, at the same power density, the 10.6 µm AR coatings on diamond substrates exhibited a lower temperature rise compared to those deposited on ZnSe substrates. Due to its high thermal conductivity, the diamond substrate is expected to exhibit reduced thermally induced surface distortion. The laser-induced damage threshold (LIDT) test results indicate that the AR coating deposited on the ZnSe substrate exhibits a damage threshold of 11,890 W/cm2, whereas the AR coating on the diamond substrate achieves a threshold of 15,287 W/cm2, representing a 28.5% improvement over the ZnSe substrate. Additionally, graphite formation occurs on the diamond substrate under high power density. These findings provide both theoretical and experimental support for the potential application of diamond materials in high-power laser systems.

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