Efficient conversion of nitrogen to nitrogen-vacancy centers in diamond particles with high-temperature electron irradiation
At a Glance
Section titled âAt a Glanceâ| Metadata | Details |
|---|---|
| Publication Date | 2020-08-19 |
| Journal | Carbon |
| Authors | Yuliya Mindarava, Rémi Blinder, Christian Laube, Wolfgang Knolle, Bernd Abel |
| Institutions | University of Tsukuba, Leibniz Institute of Surface Engineering |
| Citations | 41 |
| Analysis | Full AI Review Included |
Technical Documentation & Analysis: High-Yield NV Center Conversion via HT Electron Irradiation
Section titled âTechnical Documentation & Analysis: High-Yield NV Center Conversion via HT Electron IrradiationâExecutive Summary
Section titled âExecutive SummaryâThis research successfully demonstrates an optimized method for creating high-density, negatively-charged Nitrogen-Vacancy (NVâ») centers in diamond particles using simultaneous High-Temperature (HT) electron irradiation and annealing. This technique is critical for advancing quantum sensing and biomedical applications.
- Optimized Defect Creation: The HT irradiation method (10 MeV electrons, 800 °C annealing) significantly improved NV⻠conversion yield compared to traditional Room Temperature (RT) methods, particularly in smaller nanodiamonds (25 nm).
- Record Conversion Efficiency: Achieved a maximum P1 (substitutional nitrogen) to NV⻠conversion yield of 25 ± 3% in 2 ”m microdiamonds, a figure crucial for maximizing quantum signal strength.
- Material Quality Maintained: Despite high irradiation doses (up to 9 x 1018 cm-2), the resulting NVâ» centers maintained long spin coherence times (Tâ up to 2.7 ”s) and spin-lattice relaxation times (Tâ up to 2.6 ms), confirming minimal severe lattice damage.
- Scalability for Bulk Applications: The use of high-energy (10 MeV) electrons ensures a homogeneous vacancy distribution over large depths (>1 cm), making this technique highly scalable for processing large quantities of diamond material, including 6CCVDâs SCD and PCD wafers.
- Application Focus: The resulting high-density NVâ» materials are ideal for next-generation applications in nanoscale optical imaging, magnetic sensing, and 13C nuclear spin hyperpolarization.
Technical Specifications
Section titled âTechnical Specificationsâ| Parameter | Value | Unit | Context |
|---|---|---|---|
| Irradiation Energy | 10 | MeV | High-energy electron beam source |
| Annealing/Irradiation Temp | 800 | °C | Simultaneous High-Temperature (HT) process |
| Maximum Irradiation Dose | 9 x 1018 | cm-2 | Highest dose tested on 2 ”m particles |
| Maximum Conversion Yield | 25 ± 3 | % | P1 to NV⻠conversion (2 ”m particles) |
| Particle Sizes Tested | 25, 100, 2 | nm, ”m | Commercial HPHT Type Ib diamond powder |
| Max NV⻠Concentration | 13.5 | ppm | Achieved in 2 ”m sample (9MSY2) via CW EPR |
| NVâ» Coherence Time (Tâ) | 1.9 - 3.2 | ”s | Measured via Hahn echo (dependent on particle size/dose) |
| NVâ» Relaxation Time (Tâ) | 1.6 - 2.6 | ms | Measured via Pulsed EPR (dependent on particle size/dose) |
| Vacancy Diffusion Length (l) | ~63.8 | nm | Calculated for 2 x 1018 cm-2 dose at 800 °C |
| Secondary Defects | W16, W33 | - | Spin-1 defects increasing linearly with irradiation dose |
Key Methodologies
Section titled âKey MethodologiesâThe core innovation lies in the High-Temperature (HT) irradiation technique, which couples vacancy creation and migration into a single, highly efficient step.
- Starting Material Selection: Commercial Type Ib HPHT diamond powder was used, characterized by high initial substitutional nitrogen (P1) concentrations ranging from 5.2 ppm (25 nm) to 74 ppm (2 ”m).
- HT Irradiation Setup: Samples were placed in a quartz furnace under permanent argon flow (1 bar) and simultaneously irradiated with 10 MeV electrons. The temperature was actively regulated to 800 °C throughout the process.
- Dose Optimization: Irradiation doses were systematically varied (0.5 x 1018 cm-2 to 9 x 1018 cm-2) to map the conversion efficiency dependence, demonstrating that higher doses yield higher NVâ» concentration until saturation effects begin.
- Surface Cleaning: Post-irradiation, all samples underwent air oxidation at 620 °C for 5 hours to remove surface graphitic residues, a critical step for maintaining high spin coherence properties.
- Defect Quantification: Nitrogen (P1) and NVâ» concentrations were precisely quantified using Continuous Wave Electron Paramagnetic Resonance (CW EPR) and Pulsed EPR techniques, complemented by AFM-confocal microscopy for nanodiamonds.
- Spin Property Measurement: NVâ» spin coherence (Tâ) and spin-lattice relaxation (Tâ) times were measured using Hahn echo and Inversion/Saturation-Recovery sequences via Pulsed EPR to assess material quality and decoherence sources.
6CCVD Solutions & Capabilities
Section titled â6CCVD Solutions & Capabilitiesâ6CCVD is uniquely positioned to supply the high-quality, customized diamond materials required to replicate and advance this high-yield NVâ» creation research, transitioning it from powder experiments to scalable quantum devices.
Applicable Materials
Section titled âApplicable MaterialsâThe research highlights the need for precise control over initial nitrogen concentration (P1 centers) to maximize NVâ» conversion yield. 6CCVD offers superior control over doping and crystal quality compared to commercial HPHT powders.
| Research Requirement | 6CCVD Material Solution | Technical Advantage |
|---|---|---|
| High Initial P1 Concentration | High-Nitrogen MPCVD Polycrystalline Diamond (PCD) | Provides a Type Ib equivalent starting material with high, uniform nitrogen content necessary for high NVâ» density. Available in large formats (up to 125mm diameter). |
| High Purity, Low Defects | Optical Grade Single Crystal Diamond (SCD) | For applications requiring maximum coherence (e.g., bulk quantum sensing), 6CCVD can supply SCD with controlled nitrogen doping (Type Ib or Type Ia) for targeted NVâ» creation while minimizing secondary defects (W16, W33). |
| Surface-Sensitive Applications | Polished SCD or PCD Wafers | The paper noted surface effects dominate Tâ in 25 nm particles. 6CCVD offers ultra-smooth polishing (Ra < 1nm for SCD, < 5nm for PCD) essential for minimizing surface-induced decoherence in thin films or bulk substrates used for sensing. |
Customization Potential
Section titled âCustomization PotentialâThe scalability demonstrated by the 10 MeV electron irradiation process is perfectly matched by 6CCVDâs large-area MPCVD growth capabilities.
- Custom Dimensions: While the paper used powders, scaling this research to bulk quantum devices requires large, high-quality substrates. 6CCVD provides PCD plates up to 125mm and SCD substrates up to 10mm thick, ready for large-scale electron irradiation processing.
- Tailored Thickness: We offer SCD and PCD layers from 0.1 ”m (for thin-film sensing) up to 500 ”m, allowing researchers to precisely match the required thickness to the penetration depth of the irradiation source (10 MeV electrons penetrate >1 cm).
- Advanced Metalization: For integrating NVâ»-rich diamond into functional devices (e.g., microwave delivery structures for EPR/ODMR), 6CCVD provides in-house custom metalization services, including Au, Pt, Pd, Ti, W, and Cu deposition, directly onto the diamond surface.
Engineering Support
Section titled âEngineering SupportâThe optimization of NVâ» creation yield (25% achieved here) is highly dependent on the starting material quality and the precise irradiation/annealing recipe. 6CCVDâs in-house PhD team specializes in defect engineering and material optimization for quantum applications.
We offer consultation on:
- Selecting the optimal nitrogen concentration in the starting MPCVD material to balance high NVâ» yield against residual P1 decoherence.
- Designing custom diamond geometries (plates, wafers, or specific microstructures) suitable for high-energy electron irradiation and subsequent device fabrication.
- Analyzing the impact of surface preparation and polishing on NVâ» coherence times for similar Quantum Sensing and Hyperpolarization projects.
For custom specifications or material consultation, visit 6ccvd.com or contact our engineering team directly.
Tech Support
Section titled âTech SupportâOriginal Source
Section titled âOriginal SourceâReferences
Section titled âReferencesâ- 2013 - The nitrogen-vacancy colour centre in diamond [Crossref]
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- 2016 - Diamond quantum devices in biology [Crossref]
- 2017 - Phase-encoded hyperpolarized nanodiamond for magnetic resonance imaging
- 2019 - Controlling the fluorescence properties of nitrogen vacancy centers in nanodiamonds [Crossref]
- 2010 - Efficient production of NV colour centres in nanodiamonds using high-energy electron irradiation [Crossref]