14N Hyperfine and nuclear interactions of axial and basal NV centers in 4H-SiC - A high frequency (94 GHz) ENDOR study
At a Glance
Section titled “At a Glance”| Metadata | Details |
|---|---|
| Publication Date | 2023-09-28 |
| Journal | Journal of Applied Physics |
| Authors | Fadis F. Murzakhanov, Margarita A. Sadovnikova, G. V. Mamin, S. S. Nagalyuk, H. J. von Bardeleben |
| Institutions | Sorbonne Université, Paderborn University |
| Citations | 9 |
| Analysis | Full AI Review Included |
Technical Documentation & Analysis: 14N Hyperfine and Nuclear Interactions in 4H-SiC NV Centers
Section titled “Technical Documentation & Analysis: 14N Hyperfine and Nuclear Interactions in 4H-SiC NV Centers”This document analyzes the research article “14N Hyperfine and nuclear interactions of axial and basal NV centers in 4H-SiC: A high frequency (94 GHz) ENDOR study” (J. Appl. Phys. 134, 123906 (2023)). The analysis focuses on extracting key technical data and leveraging 6CCVD’s capabilities in MPCVD diamond growth to support and extend this advanced quantum research.
Executive Summary
Section titled “Executive Summary”The following is a high-density summary of the research findings and 6CCVD’s core value proposition for quantum technology applications:
- Core Achievement: Determined the complete spin-Hamiltonian parameters (Hyperfine Interaction, HFI, and Nuclear Quadrupole Interaction, NQI) for all four inequivalent Nitrogen-Vacancy (NV) center configurations (NVkk, NVhh, NVhk, NVkh) in 4H-SiC.
- Methodology: Utilized high-frequency (94 GHz) Electron-Nuclear Double Resonance (ENDOR) spectroscopy combined with Density Functional Theory (DFT) calculations to achieve kHz resolution necessary for resolving weak interactions.
- Quantum Relevance: The precise knowledge of electron-nuclear interaction parameters is critical for establishing quantum protocols, specifically for polarization transfer from the electron spin to the 14N nuclear spin, enabling quantum memory nodes.
- Key Finding: Observed differences in HFI and NQI parameters between the four NV configurations, rationalized by subtle distinctions in local atomic structure, suggesting each configuration may act as a separate optically addressable qubit.
- 6CCVD Value Proposition: While SiC NV centers are promising, the ultimate performance metrics (ultra-long coherence times, T2) are achieved using the NV- center in Single Crystal Diamond (SCD).
- Sales Driver: 6CCVD supplies ultra-high purity SCD substrates, ready for precise ion implantation and annealing, offering the superior material platform required to extend this foundational research into scalable, high-coherence quantum devices.
Technical Specifications
Section titled “Technical Specifications”The following table summarizes the critical experimental and derived data points from the research:
| Parameter | Value | Unit | Context |
|---|---|---|---|
| Host Material Polytype | 4H-SiC | N/A | Commercial n-type bulk crystal |
| Initial Nitrogen Concentration | 2 x 1017 | cm-3 | Sample doping level |
| Irradiation Particle | Proton | N/A | Used for VSi defect generation |
| Irradiation Energy | 12 | MeV | High-energy proton source |
| Irradiation Fluence | 1 x 1016 | cm-2 | Dose used for defect creation |
| Annealing Temperature | 900 | °C | Optimal temperature for NV formation |
| Spectrometer Frequency | 94 (W-band) | GHz | ESE ESR/ENDOR measurement frequency |
| Measurement Temperature | 150 | K | Experimental temperature |
| NVhh Quadrupole Splitting (P) | 1.89 (± 0.05) | MHz | Nuclear Quadrupole Interaction (NQI) |
| NVhh Hyperfine Constant (A||) | -1.165 | MHz | Axial Electron-Nuclear HFI |
| NVkk Quadrupole Splitting (P) | 1.81 | MHz | Axial NQI (slightly smaller than NVhh) |
| NVkk Hyperfine Constant (A||) | 1.14 | MHz | Axial HFI (slightly smaller than NVhh) |
| NVkh Hyperfine Constant (A||) | -1.05 | MHz | Basal HFI |
| NVhk Hyperfine Constant (A||) | -0.87 | MHz | Basal HFI |
Key Methodologies
Section titled “Key Methodologies”The experimental approach combined material processing (defect generation) with advanced high-frequency spectroscopy and computational modeling:
- Substrate Selection: Used commercial n-type, (0001) face 4H-SiC bulk crystal with a native nitrogen concentration of 2 x 1017 cm-3.
- Defect Creation: Silicon vacancies (VSi) were generated via high-energy (12 MeV) proton irradiation at a fluence of 1 x 1016 cm-2.
- NV Center Formation: Thermal annealing was performed at T = 900 °C, allowing mobile VSi defects to complex with carbon-substituted nitrogen atoms, forming stable NV centers (NVCVSi).
- ESR Detection: Electron Spin Echo-Detected (ESE) ESR measurements were conducted at W-band (94 GHz) and T = 150 K to establish the resonance magnetic fields of the fine structure transitions.
- ENDOR Spectroscopy: Pulsed ENDOR measurements utilized a Mims-pulse sequence (π/2 - τ - π - T - π/2 - RF π-pulse - π/2 - ESE) to measure NMR transitions with kHz resolution, allowing precise determination of HFI and NQI parameters.
- Computational Modeling (DFT): Density Functional Theory (DFT) using the PBE functional and GIPAW module was employed to calculate 14N electron-nuclear coupling parameters and rationalize the observed differences based on local atomic structure deviations.
6CCVD Solutions & Capabilities
Section titled “6CCVD Solutions & Capabilities”This research provides foundational data for solid-state qubits. While SiC is a viable platform, the highest performance quantum memory and sensing applications rely on the superior coherence properties of the NV center in diamond. 6CCVD is uniquely positioned to supply the necessary materials and processing capabilities to advance this research using the diamond platform.
| Applicable Materials & Requirements | 6CCVD Solution & Capability | Engineering Advantage |
|---|---|---|
| High-Coherence Qubit Platform | Optical Grade Single Crystal Diamond (SCD): SCD grown via MPCVD with ultra-low native nitrogen (< 1 ppb) and minimal strain. | Provides the longest known spin coherence times (T2), essential for extending quantum protocols beyond SiC limitations. |
| Precise Defect Generation | Custom SCD Substrates for Implantation: SCD plates (0.1 µm to 500 µm thickness) optimized for external ion implantation (e.g., 14N or 15N) to control NV density and depth. | Enables deterministic creation of single NV centers or high-density ensembles, replicating the defect generation methodology used in the SiC study. |
| Large-Scale Device Development | Large Format PCD Wafers: Polycrystalline Diamond (PCD) plates up to 125 mm diameter, suitable for scalable quantum sensor arrays or high-throughput processing. | Offers a cost-effective, large-area alternative for applications where ensemble coherence (T2*) is sufficient. |
| Integration of MW Control Structures | In-House Custom Metalization: Internal capability to deposit thin films (Au, Pt, Pd, Ti, W, Cu) for creating microwave striplines or electrodes required for high-frequency (94 GHz) ENDOR/ESR setups. | Ensures robust, high-quality metal contacts necessary for efficient MW delivery and coherent spin control. |
| Optimized Optical Readout | Precision Polishing Services: SCD substrates polished to Ra < 1 nm, ensuring minimal surface roughness for high-efficiency optical readout (PL/ODMR) and integration with nanophotonic structures. | Reduces scattering losses, critical for maximizing the signal-to-noise ratio in single-qubit experiments. |
| Material Optimization for HFI/NQI Studies | Boron-Doped Diamond (BDD): Available for electrochemistry or specific charge state control studies, offering a complementary material platform for quantum research. | Allows researchers to explore the impact of doping on NV charge state stability and local electric fields (EFG), relevant to NQI parameters. |
Engineering Support
Section titled “Engineering Support”6CCVD’s in-house PhD team specializes in optimizing MPCVD growth parameters to control impurity incorporation (e.g., nitrogen, boron) and minimize strain, which directly impacts the Zero-Field Splitting (ZFS) and coherence times of solid-state defects. We can assist researchers transitioning from SiC to diamond or optimizing diamond recipes for similar NV Center Hyperfine Interaction projects.
For custom specifications or material consultation, visit 6ccvd.com or contact our engineering team directly.
View Original Abstract
The nitrogen-vacancy (NV) centers (NCVSi)− in 4H silicon carbide (SiC) constitute an ensemble of spin S = 1 solid state qubits interacting with the surrounding 14N and 29Si nuclei. As quantum applications based on a polarization transfer from the electron spin to the nuclei require the knowledge of the electron-nuclear interaction parameters, we have used high-frequency (94 GHz) electron-nuclear double resonance spectroscopy combined with first-principles density functional theory to investigate the hyperfine and nuclear quadrupole interactions of the basal and axial NV centers. We observed that the four inequivalent NV configurations (hk, kh, hh, and kk) exhibit different electron-nuclear interaction parameters, suggesting that each NV center may act as a separate optically addressable qubit. Finally, we rationalized the observed differences in terms of distinctions in the local atomic structures of the NV configurations. Thus, our results provide the basic knowledge for an extension of quantum protocols involving the 14N nuclear spin.
Tech Support
Section titled “Tech Support”Original Source
Section titled “Original Source”References
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