Abrasive wear damages observation in engineering ceramics using micro-Raman tomography
At a Glance
Section titled âAt a Glanceâ| Metadata | Details |
|---|---|
| Publication Date | 2022-12-31 |
| Journal | Journal of Advanced Mechanical Design Systems and Manufacturing |
| Authors | Teppei Onuki, Kazuki Kaneko, Hirotaka Ojima, Jun Shimizu, Libo ZHOU |
| Institutions | Ibaraki University |
| Analysis | Full AI Review Included |
Technical Documentation & Analysis: Precision Diamond Surfaces for Advanced Raman Tomography
Section titled âTechnical Documentation & Analysis: Precision Diamond Surfaces for Advanced Raman TomographyâThis document analyzes the research paper âAbrasive wear damages observation in engineering ceramics using micro-Raman tomographyâ and connects the findings directly to 6CCVDâs capabilities in MPCVD diamond material science, specifically focusing on how high-quality Single Crystal Diamond (SCD) and Polycrystalline Diamond (PCD) surfaces can overcome the optical limitations identified in ceramic materials.
Executive Summary
Section titled âExecutive SummaryâThe study validates Micro-Raman Tomographic Imaging (mRTI) for subsurface wear damage analysis in ceramics but highlights critical limitations related to optical diffusion in polycrystalline materials. 6CCVDâs ultra-precision diamond materials directly address these limitations, enabling deeper, more accurate spectroscopic analysis.
- Core Challenge: Optical diffusion in polycrystalline ceramics (Alumina) severely restricts the effective mRTI measurement depth (initially 4-8 ”m).
- Solution Demonstrated: Precision surface polishing using diamond abrasives (#800) reduced surface roughness ($R_a$) from 600 nm to 200 nm, significantly reducing light diffusion.
- Key Achievement: Optimized polishing extended the effective measurement depth range across the full 17 ”m scan depth, confirming the necessity of superior surface quality.
- Material Superiority: The paper notes that single-crystal materials (like sapphire, analogous to 6CCVDâs SCD) achieved deeper penetration (up to 20 ”m) even with rougher surfaces, confirming the optical advantage of single-crystal structures.
- 6CCVD Value Proposition: We provide SCD and PCD materials with guaranteed surface roughness (Ra < 1 nm for SCD), eliminating the optical diffusion issues that plague polycrystalline ceramics and ensuring maximum effective measurement depth for advanced spectroscopic techniques.
- Critical Process Control: The research emphasizes that polishing must be optimized to reduce diffusion without overwriting the original wear damageâa requirement met by 6CCVDâs precision mechanical polishing capabilities.
Technical Specifications
Section titled âTechnical SpecificationsâThe following hard data points were extracted from the mRTI experiment and material characterization:
| Parameter | Value | Unit | Context |
|---|---|---|---|
| Sample Material Purity | 96 | % | Commercial Alumina Ceramic (Al2O3) |
| Initial Surface Roughness (Ra) | 600 | nm | Arithmetic average roughness of initial surface |
| Polished Surface Roughness (#400) (Ra) | 300 | nm | Achieved via #400 diamond lapping film |
| Polished Surface Roughness (#800) (Ra) | 200 | nm | Achieved via #800 diamond lapping film |
| Initial Max Measurable Depth | 4 to 8 | ”m | Limited by light diffusion in polycrystalline material |
| Improved Max Measurable Depth | 17 | ”m | Effective over entire scan range after #800 polishing |
| Raman Peak Used (Alumina) | 417 | cm-1 | Corresponds to A1g vibration mode |
| Laser Wavelength | 532 | nm | mRTI measurement condition |
| Laser Power | 10 | mW | mRTI measurement condition |
| Confocal Aperture | 25 | ”m | Pin hole diameter |
| Grating Density | 1800 | lines/mm | Spectral resolution approximately 2 cm-1 |
| Objective Lens Numerical Aperture (NA) | 0.9 | N/A | Magnification x100 |
| Exposure Time per Point | 16 | sec. | Required for high-resolution 2D depth-slice scanning |
| Refractive Index (Alumina) | 1.76 | N/A | Used for depth correction in mRTI scanning |
Key Methodologies
Section titled âKey MethodologiesâThe experiment focused on evaluating the influence of surface quality on mRTI depth penetration in polycrystalline ceramics.
- Sample Selection: Commercial alumina ceramic plates (96% purity, 20 mm x 20 mm x 1 mm) were used as the measurement samples.
- Initial Characterization: Surface topography and roughness (Ra â 600 nm) were measured using an optical surface profiler (Zygo New View 2000).
- Surface Treatment Simulation: Three surface conditions were prepared: initial surface, polished with #400 diamond abrasive lapping film, and polished with #800 diamond abrasive lapping film. Polishing was performed by hand for 15 minutes.
- mRTI Setup: A DXR Raman microscope (Thermo Fisher Scientific) was utilized, employing a 532 nm laser at 10 mW power, focused through a NA 0.9 objective lens.
- Data Acquisition: Raman spectra were acquired using a 25 ”m confocal pinhole and an 1800 lines/mm grating, with a 16-second exposure time per point.
- Depth-Slice Scanning: 2D scanning was conducted over a 24 ”m horizontal range (1 ”m pitch) and a 17 ”m depth range (0.85 ”m pitch, corrected using the alumina refractive index of 1.76).
- Damage Quantification: Tomographic images were generated by fitting the Raman spectra to the Lorentzian function, extracting peak intensity, peak width (indicating crystal lattice disorder), and peak shift (indicating residual strain/stress).
6CCVD Solutions & Capabilities
Section titled â6CCVD Solutions & CapabilitiesâThe research confirms that surface quality is the primary limiting factor for deep subsurface analysis using optical techniques like mRTI in polycrystalline materials. 6CCVDâs expertise in growing and finishing high-purity MPCVD diamond provides the ideal platform for replicating and extending this research into high-performance materials.
Applicable Materials
Section titled âApplicable Materialsâ| Material | Application Focus | Technical Rationale |
|---|---|---|
| Optical Grade Single Crystal Diamond (SCD) | Advanced Spectroscopic Windows, High-Resolution mRTI Substrates, Quantum Sensing | SCD is the ultimate single-crystal material. Unlike polycrystalline alumina, SCD exhibits negligible light diffusion, maximizing the effective measurement depth (analogous to the superior performance noted for single-crystal sapphire). |
| Polycrystalline Diamond (PCD) | Industrial Wear Components, Large-Area Tribology Studies, High-Hardness Substrates | Ideal for replicating the high-wear conditions studied. Our PCD can be polished to Ra < 5 nm across inch-sized wafers, providing a superior, low-diffusion surface compared to the 200 nm achieved on alumina. |
| Boron-Doped Diamond (BDD) | Electrochemical Sensing, Conductive Wear Studies | If the research were extended to include electrical or electrochemical wear mechanisms, BDD offers high conductivity combined with diamondâs extreme hardness and chemical inertness. |
Customization Potential for Spectroscopic Research
Section titled âCustomization Potential for Spectroscopic ResearchâThe paper highlights the critical need for precision mechanical polishing using diamond abrasives. 6CCVD specializes in this exact process, ensuring materials are delivered ready for high-sensitivity optical measurement.
| Research Requirement | 6CCVD Customization Capability |
|---|---|
| Ultra-Low Roughness Surfaces | We guarantee SCD surfaces with Ra < 1 nm and large-area PCD surfaces with Ra < 5 nm. This level of polish is essential to minimize surface light scattering and maximize mRTI depth penetration. |
| Custom Dimensions & Thickness | We offer PCD plates up to 125 mm in diameter and custom SCD/PCD thicknesses ranging from 0.1 ”m to 500 ”m, allowing researchers to design components or substrates precisely for their experimental setup. |
| Integrated Metalization | For applications requiring electrical contacts or thermal management (e.g., integrated heating elements for wear testing), we offer in-house metalization (Au, Pt, Pd, Ti, W, Cu) patterned to custom specifications. |
| Damage-Free Preparation | Our in-house processing ensures that laser cutting and polishing are performed under optimized conditions, preventing the introduction of residual strain or lattice damage that could âoverwriteâ the wear damage being studied, as cautioned by the authors. |
Engineering Support
Section titled âEngineering Supportâ6CCVDâs in-house PhD team provides expert consultation to ensure material selection and preparation are optimized for demanding optical and spectroscopic applications. We can assist researchers in defining the optimal surface finish and material grade (SCD vs. PCD) required for similar subsurface wear damage analysis projects, guaranteeing that the material itself does not become the limiting factor in measurement depth or signal quality.
For custom specifications or material consultation, visit 6ccvd.com or contact our engineering team directly.
View Original Abstract
Micro Raman tomographic imaging (mRTI) is an excellent measurement technique that can nondestructively measure and image the fracture state of the crystal lattice inside materials with a high spatial resolution. mRTI has been successfully used for translucent materials such as wide bandgap semiconductor wafers. The applicability of this measurement method was evaluated by observing the wear damage in polycrystalline industrial ceramics materials. The influence of optical diffusion on the surface and inside of polycrystalline materials is a concern for the internal measurements by the optical beam. The quality degradation of spectral signals due to disturbances in the optical beam was confirmed by mRTI measurements on a commercial alumina plate. The application of surface polishing treatment was attempted to reduce the influence of surface optical diffusion. Three kinds of the surfaces were observed by mRTI, as the initial surface of the alumina plate, polished with #400 and #800 diamond abrasive lapping film, respectively. It was confirmed that the effective measurement depth range can be extended by reducing the surface roughness. However, we confirmed that excessive surface polishing may overwrite the damage on the measurement surface, making it difficult to observe the original damage.