Low-Power Laser Graphitization of High Pressure—High Temperature Nanodiamond Films
At a Glance
Section titled “At a Glance”| Metadata | Details |
|---|---|
| Publication Date | 2020-05-11 |
| Journal | Applied Sciences |
| Authors | Konstantin G. Mikheev, T. N. Mogileva, Arseniy E. Fateev, Nicholas Nunn, Olga Shenderova |
| Institutions | Adámas Nano (United States), North Carolina State University |
| Citations | 14 |
| Analysis | Full AI Review Included |
Executive Summary
Section titled “Executive Summary”This research demonstrates a novel, low-power method for the structural modification and graphitization of High-Pressure High-Temperature (HP-HT) nanodiamond (ND) films.
- Core Achievement: Successful laser-induced graphitization (sp3 to sp2 carbon conversion) of 150 nm HP-HT ND films using a continuous-wave (CW) 633 nm He-Ne laser, requiring less than 10 mW of optical power.
- Threshold Intensity: Graphitization initiates sharply when the focused laser intensity exceeds a threshold of approximately 33 kW/cm2.
- Mechanism: The process is driven by a two-step sequential resonance absorption mechanism involving Ni- and Ni-N-related impurity centers, leading to photoionization and the generation of free electrons.
- Observation: The structural change is accompanied by transient green up-conversion luminescence (461-535 nm region), confirming the activation and ionization of these impurity centers.
- Spatial Selectivity: Modification occurs primarily when the film is moved relative to the laser spot, indicating a non-uniform distribution of the active impurity centers within the ND particles.
- Structural Result: The modified area exhibits a significant change in morphology, characterized by a surface notch (150 nm deep) and surrounding parallel ridges (100 nm high).
- Implication: This technique provides a method for the selective destruction of impurity-rich ND particles, opening possibilities for laser-assisted purification of HP-HT nanodiamonds.
Technical Specifications
Section titled “Technical Specifications”| Parameter | Value | Unit | Context |
|---|---|---|---|
| Nanodiamond Source Material | HP-HT monocrystals | N/A | Average particle size 150 nm. |
| Film Thickness (Modification) | 20 | µm | Formed on quartz substrate. |
| Laser Type | CW He-Ne | N/A | Continuous wave excitation source. |
| Laser Wavelength | 633 | nm | Used for excitation and modification. |
| Maximum Laser Power | 8.4 | mW | Output using 100x objective. |
| Graphitization Threshold Intensity | ~33 | kW/cm2 | Minimum intensity required for sp3 to sp2 conversion. |
| Maximum Intensity Used | 65 | kW/cm2 | Used for stationary irradiation tests. |
| Laser Beam Waist Diameter (100x) | 4.1 | µm | 1/e2 level. |
| Laser Written Line Width | ~5 | µm | Transverse width of the blackened segment. |
| Unmodified Diamond Raman Shift | 1331 | cm-1 | Characteristic HP-HT ND peak. |
| sp2 Carbon Raman Shifts | 1320 and 1580 | cm-1 | Typical broad lines for graphitic carbon. |
| AFM Notch Depth (Blackened Area) | ~150 | nm | Depth of the laser-induced trench. |
| AFM Ridge Height (Blackened Area) | ~100 | nm | Height of material raised adjacent to the notch. |
| Extinction Spectrum Maximum | 208 | nm | Corresponds to 5.96 eV (diamond bandgap). |
| Up-Conversion Luminescence Peaks | 485 and 528-529 | nm | Associated with Ni- and Ni-N-related centers (blue-green emission). |
| Substitutional Nitrogen Concentration | 100-300 | ppm | Impurity level in HP-HT ND. |
Key Methodologies
Section titled “Key Methodologies”- Sample Preparation: HP-HT nanodiamond particles (150 nm average size) were dispersed in deionized water. Films (20 µm thick) were formed by drop-casting the aqueous suspension onto quartz substrates and drying at room temperature.
- Irradiation Setup: Experiments utilized a Horiba HR800 Raman spectrometer setup with a CW He-Ne laser (633 nm) as the excitation source. The beam was focused using 10x, 50x, or 100x objectives.
- Laser Modification: Films were moved relative to the focused laser spot using a coordinate table to “write” patterns (lines, squares, triangles). Modification was tested in ambient air and Ar atmosphere.
- In-Situ Observation: Green up-conversion luminescence accompanying the graphitization event was visually observed and recorded using a photo camera, confirming the activation of Ni-related photoluminescent centers.
- Structural Analysis (XRD): X-ray diffraction confirmed the high-quality diamond structure of the starting material (peaks corresponding to {111}, {220}, {311} planes).
- Spectroscopic Analysis (Raman): Raman spectra were used to confirm the structural transformation: the diamond peak (1331 cm-1) disappeared in the blackened region, replaced by broad sp2 carbon peaks (1320 and 1580 cm-1).
- Morphological Analysis (AFM/SEM): Atomic Force Microscopy (AFM) and Scanning Electron Microscopy (SEM) were used to characterize the surface morphology before and after laser treatment, revealing the granular structure and the formation of laser-induced notches and ridges.
Commercial Applications
Section titled “Commercial Applications”The ability to selectively modify nanodiamonds based on their impurity content using low-power visible lasers has implications for several advanced materials and manufacturing sectors:
- Nanodiamond Purification: The targeted destruction (graphitization) of nanodiamonds containing Ni- and N-related defects enables a laser-assisted extraction process to yield higher purity HP-HT nanodiamonds, critical for sensitive applications.
- Micro-Optics and Patterning: Localized sp3 to sp2 conversion allows for the direct writing of conductive or absorptive micro-patterns on insulating ND films, useful for fabricating micro-scale optical structures, diffractive elements, or embedded electrical contacts.
- Quantum Sensing Materials: While the goal here is destruction, the detailed understanding of the resonant absorption and ionization dynamics of Ni- and N-related centers (which often act as precursors to quantum defects like NV centers) is valuable for controlling defect creation and stability in quantum sensing applications.
- Advanced Composites: Creating localized conductive pathways (sp2 carbon) within bulk insulating ND matrices could be used to engineer novel thermal or electrical properties in composite materials.
View Original Abstract
Laser-induced graphitization of 100 nm monocrystals of diamond particles synthesized by high-pressure high-temperature (HP-HT) methods is not typically observed. The current study demonstrates the graphitization of 150 nm HP-HT nanodiamond particles in ca. 20-μm-thick thin films formed on a glass substrate when the intensity of a focused 633 nm He-Ne laser exceeds a threshold of ~ 33 kW/cm2. Graphitization is accompanied by green luminescence. The structure and morphology of the samples were investigated before and after laser excitation while using X-ray diffraction (XRD), Raman spectroscopy, atomic force (AFM), and scanning electron microscopy (SEM). These observations are explained by photoionization of [Ni-N]- and [N]-centers, leading to the excitation of electrons to the conduction band of the HP-HT nanodiamond films and an increase of the local temperature of the sample, causing the transformation of sp3 HP-HT nanodiamonds to sp2-carbon.
Tech Support
Section titled “Tech Support”Original Source
Section titled “Original Source”References
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