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Femtosecond-Laser Nanostructuring of Black Diamond Films under Different Gas Environments

MetadataDetails
Publication Date2020-12-17
JournalMaterials
AuthorsM. Girolami, A. Bellucci, Matteo Mastellone, S. Orlando, Valerio Serpente
InstitutionsInstitute of Nanostructured Materials, Sapienza University of Rome
Citations11
AnalysisFull AI Review Included

This research validates a cost-effective, ambient-pressure manufacturing workflow for high-performance black diamond films, traditionally requiring complex Ultra-High Vacuum (UHV) conditions.

  • Core Achievement: Demonstrated that femtosecond (fs) laser nanostructuring of polycrystalline diamond under a constant Helium (He) flow achieves optical properties nearly identical to those fabricated in UHV.
  • Value Proposition: Eliminates the need for expensive and complex UHV systems, paving the way for large-scale, cost-effective production of black diamond solar absorbers.
  • Performance Metric: The He-treated film (TM3-He) achieved a solar absorptance (αs) of 86.2%, closely matching the optimal UHV reference value of 88.4%.
  • Mechanism of Success: He flow ensures a uniform distribution of Laser Induced Periodic Surface Structures (LIPSS) across the polycrystalline surface, crucial for efficient light trapping.
  • Failure Analysis (Air/N2): Treatments under compressed air or N2 flow resulted in irregular, terraced surfaces with deep cracks along grain boundaries, leading to poor LIPSS uniformity and significantly lower αs (~79%).
  • Structural Integrity: The He-treated sample exhibited compressive stress (Raman peak upshift), consistent with optimal UHV-fabricated black diamond films, indicating high structural quality.
ParameterValueUnitContext
Target MaterialPolycrystalline CVD DiamondN/AThermal Management (TM) Grade
Laser Wavelength (λfs)800nmTi:sapphire system
Pulse Duration~100fsUltrafast regime
Repetition Rate (f)1kHzFixed parameter
Laser Spot Diameter (2w)150µm1/e2 width
Single Pulse Fluence (Φp)4.44J/cm2Above ablation threshold (~3 J/cm2)
Total Accumulated Fluence (ΦA)5.0kJ/cm2Optimal fluence for 1D LIPSS
Horizontal Scan Speed (vx)1mm/sRaster pattern speed
LIPSS Periodicity (Ī›)170 ± 10nmMeasured structure size (Theoretical: 166 nm)
Solar Absorptance (αs) - He86.2%Best ambient condition result (TM3-He)
Solar Absorptance (αs) - UHV Ref.88.4%Previous optimal UHV result
Solar Absorptance (αs) - Air79.1%Result for TM1-air
Diamond Raman Peak (TM3-He)1335.1cm-1Compressive stress (Upshifted from 1332.0 cm-1)
Diamond Raman Peak (TM1-Air)1326.3cm-1Tensile stress (Downshifted)
LIPSS Depth480 ± 20nmInferred from tilted SEM images

The fabrication process utilized a linearly polarized fs-pulsed laser system in a raster scanning pattern on polycrystalline CVD diamond samples at ambient pressure.

  1. Pre-Cleaning: Samples were subjected to a standard cleaning procedure using a strongly oxidizing mixture (HNO3:H2SO4:HClO4, 1:1:1 volume ratio) at boiling point for 15 minutes, followed by ultrasonic cleaning in acetone and 2-propanol.
  2. Laser Setup: A Ti:sapphire laser system (800 nm, 100 fs, 1 kHz) was used, focused to a 150 µm spot diameter.
  3. Scanning Parameters: The laser scanned an 8 x 8 mm2 area at a constant speed (1 mm/s) with a vertical shift (Ī”y = 20 µm) to ensure a precise total accumulated fluence (ΦA) of 5.0 kJ/cm2.
  4. Gas Environment Control: A constant flow of gas (Compressed Air, N2, or He) was directed towards the sample surface. The flow angle was maintained close to 90° to the surface normal to prevent spatially dependent boundary layer thickness.
  5. Post-Treatment: Samples were cleaned again using the oxidizing mixture to remove debris generated by the ablation process.
  6. Morphological Analysis (SEM): FE-SEM was used to evaluate LIPSS formation and uniformity. A thin (~2 nm) Au coating was applied prior to SEM to prevent sample charging.
  7. Structural Analysis (Raman): Raman spectroscopy (514.5 nm Ar+ laser) was performed to assess structural modifications, crystalline quality (FWHM), and internal stress (peak shift).
  8. Optical Analysis (Spectrophotometry): Absorptance (α) spectra were derived from measured transmittance (Ļ„) and hemispherical reflectance (ρ) in the 0.25-2.5 µm range, used to calculate the solar absorptance (αs) under AM 1.5 global-tilt irradiance.

This technology is highly relevant for applications requiring robust, high-efficiency solar absorption and thermal stability, particularly where manufacturing cost reduction is critical.

  • Concentrated Solar Power (CSP) Receivers: Black diamond films offer outstanding solar absorptance (αs > 85%) across the solar spectrum, making them ideal for high-efficiency solar thermal collectors.
  • Photon-Enhanced Thermionic Emission (PETE) Devices: Black diamond is suitable for use as a cathode material in PETE solar cells, which operate at very high temperatures (Ref. [4-6]).
  • Solar Thermionic-Thermoelectric Generators (ST2G): Used as the primary solar absorber component in hybrid energy conversion systems that require materials stable at extreme heat (Ref. [37]).
  • High-Temperature Electronics/Coatings: Diamond’s inherent thermal management properties, combined with enhanced optical absorption, make it valuable for protective or functional coatings in harsh thermal environments.
  • Industrial Laser Processing: The successful transition from UHV to ambient He flow enables the integration of black diamond fabrication into standard, high-throughput industrial laser processing lines, reducing capital expenditure and operational complexity.
View Original Abstract

Irradiation of diamond with femtosecond (fs) laser pulses in ultra-high vacuum (UHV) conditions results in the formation of surface periodic nanostructures able to strongly interact with visible and infrared light. As a result, native transparent diamond turns into a completely different material, namely ā€œblackā€ diamond, with outstanding absorptance properties in the solar radiation wavelength range, which can be efficiently exploited in innovative solar energy converters. Of course, even if extremely effective, the use of UHV strongly complicates the fabrication process. In this work, in order to pave the way to an easier and more cost-effective manufacturing workflow of black diamond, we demonstrate that it is possible to ensure the same optical properties as those of UHV-fabricated films by performing an fs-laser nanostructuring at ambient conditions (i.e., room temperature and atmospheric pressure) under a constant He flow, as inferred from the combined use of scanning electron microscopy, Raman spectroscopy, and spectrophotometry analysis. Conversely, if the laser treatment is performed under a compressed air flow, or a N2 flow, the optical properties of black diamond films are not comparable to those of their UHV-fabricated counterparts.

  1. 2015 - Absorptance enhancement in fs-laser-treated CVD diamond [Crossref]
  2. 2016 - Infrared absorption of fs-laser textured CVD diamond [Crossref]
  3. 2016 - Optimization of black diamond films for solar energy conversion [Crossref]
  4. 2017 - Graphite distributed electrodes for diamond-based photon-enhanced thermionic emission solar cells [Crossref]
  5. 2016 - Black diamond for solar energy conversion [Crossref]
  6. 2012 - Femtosecond laser-induced periodic surface structures [Crossref]
  7. 2017 - Laser-induced periodic surface structures on bismuth thin films with ns laser pulses below ablation threshold [Crossref]
  8. 2017 - Femtosecond laser induced robust periodic nanoripple structured mesh for highly efficient oil-water separation [Crossref]
  9. 2020 - Femtosecond laser fabrication of LIPSS-based waveplates on metallic surfaces [Crossref]