Subnanotesla Magnetometry with a Fiber-Coupled Diamond Sensor
At a Glance
Section titled âAt a Glanceâ| Metadata | Details |
|---|---|
| Publication Date | 2020-10-30 |
| Journal | Physical Review Applied |
| Authors | R. L. Patel, Li Zhou, Angelo Frangeskou, G. A. Stimpson, Ben G. Breeze |
| Institutions | Engineering and Physical Sciences Research Council, Element Six (United Kingdom) |
| Citations | 62 |
| Analysis | Full AI Review Included |
Technical Documentation & Analysis: Fiber-Coupled Diamond Magnetometry
Section titled âTechnical Documentation & Analysis: Fiber-Coupled Diamond MagnetometryâExecutive Summary
Section titled âExecutive SummaryâThis research demonstrates a significant advancement in compact, high-sensitivity magnetometry using ensemble Nitrogen Vacancy (NV) centers in diamond, specifically targeting applications like Magnetocardiography (MCG).
- Record Sensitivity: Achieved a sensitivity of (310 ± 20) pT/âHz in the 10-150 Hz range, representing the best reported sensitivity for a fiber-coupled diamond magnetometer using applied test fields.
- Core Material: The sensor relies on a 4 mm x 4 mm x 0.6 mm, (100)-oriented Single Crystal Diamond (SCD) enriched to 99.995% 12C, grown via Chemical Vapor Deposition (CVD).
- Compact Design: The fiber-coupled setup allows the sensor head to be brought within 2 mm of the object under study, crucial for high-mobility medical diagnostic techniques.
- Methodology: Sensitivity was achieved using continuous wave Optically Detected Magnetic Resonance (ODMR) combined with square-wave frequency modulation and lock-in detection.
- Performance Gap: The achieved sensitivity is approximately six times worse than the estimated photon shot-noise limit (50 pT/âHz), primarily due to poor photon collection efficiency (0.03% conversion efficiency) caused by diamondâs high refractive index (nd = 2.42).
- Future Optimization: Improvements require advanced optical integration (e.g., total internal reflection lenses or waveguides) and more homogeneous microwave driving fields.
Technical Specifications
Section titled âTechnical Specificationsâ| Parameter | Value | Unit | Context |
|---|---|---|---|
| Achieved Sensitivity (Applied Field) | 310 ± 20 | pT/âHz | Measured using known test fields (10-150 Hz range) |
| Photon Shot Noise Limit (Estimated) | 50 | pT/âHz | Theoretical limit based on collected fluorescence (1.2x1015 photons/s) |
| Diamond Material | Single Crystal CVD | N/A | 99.995% 12C enriched |
| Diamond Dimensions | 4 x 4 x 0.6 | mm | (100)-orientation |
| NV- Concentration | 4.6 | ppm | Negatively charged Nitrogen Vacancy centers |
| Excitation Wavelength | 532 | nm | Green laser excitation |
| Excitation Power (Used) | 1 | W | Used to reduce laser noise |
| Zero-Field Splitting (NVC) | ~2.87 | GHz | Room temperature operation |
| Measurement Contrast (C) | 1.76 | % | Extracted from ODMR spectrum |
| Linewidth (ÎΜ) | 1.11 | MHz | Extracted from ODMR spectrum |
| Optimal Microwave Power | ~0.8 | W | Power after amplification |
| Refractive Index (nd) | 2.42 | N/A | Primary cause of low photon collection efficiency |
Key Methodologies
Section titled âKey MethodologiesâThe sub-nanotesla sensitivity was achieved using a highly optimized continuous wave ODMR setup focusing on noise reduction and precise microwave control.
- Optical Excitation and Noise Cancellation:
- A 1 W, 532 nm laser beam was focused into a 5 m, 400 ”m core optical fiber (0.22 N.A.).
- Laser intensity noise was actively cancelled using a Thorlabs PDB450A balanced detector, sampling approximately 1% of the incident beam.
- Fiber-to-Diamond Coupling:
- The fiber output was collimated and focused onto the diamond using a pair of adjustable aspheric lenses (Thorlabs C171TMD-B and C330TMD-B). The same lenses collected the resulting fluorescence.
- Microwave Generation and Delivery:
- Microwave excitation (2-4 GHz range) was provided by an Agilent N5172B source and amplified by a Mini-Circuits ZHL-16W-43-S+ amplifier.
- Microwaves were delivered via a 5 mm copper loop deposited onto an aluminum prototyping board, which also served for heat management.
- Signal Optimization:
- Hyperfine excitation was utilized by mixing a 2.158 MHz sinewave to improve ODMR contrast.
- Microwaves were square-wave frequency modulated (FM depth 300 kHz, FM frequency 3.0307 kHz) to maximize the zero-crossing slope.
- Magnetic Alignment:
- A permanent rare earth magnet was aligned to the (111) crystallographic orientation to maximize the projection of the external field onto the NVC symmetry axis.
- Detection:
- The signal was processed by a Zurich MFLI DC - 500 kHz lock-in amplifier (LIA). Sensitivity was determined by analyzing 160 one-second Fast-Fourier Transforms (FFTs) of the fluorescence signal monitored at the zero-crossing point.
6CCVD Solutions & Capabilities
Section titled â6CCVD Solutions & CapabilitiesâThe successful replication and extension of this sub-nanotesla magnetometry research hinges on the availability of ultra-high-quality, custom-engineered diamond substrates. 6CCVD is uniquely positioned to supply the necessary materials and fabrication services required for next-generation NV-based quantum sensors.
| Research Requirement | 6CCVD Applicable Materials | Customization Potential & Sales Advantage |
|---|---|---|
| High-Purity Substrate | Optical Grade SCD (Single Crystal Diamond): We supply low-strain, high-purity MPCVD SCD, essential for maximizing the NV center coherence time (T2). | We can provide isotopically enriched 12C SCD (as used in this paper) to minimize decoherence from 13C nuclear spins, ensuring optimal quantum performance. |
| Custom Dimensions & Thickness | SCD Plates/Wafers & Substrates: The paper used 4 mm x 4 mm x 0.6 mm. We offer custom dimensions up to 125 mm (PCD) and precise thickness control for SCD (0.1 ”m - 500 ”m) and substrates (up to 10 mm). | Precision Laser Cutting: Enables the fabrication of sensor heads with exact geometries required for compact fiber coupling and integration within 2 mm of the target object. |
| Optical Integration & Efficiency | Ultra-Low Roughness Polishing: SCD polishing capability to Ra < 1 nm. | The paper identifies collection efficiency (0.03%) as the biggest limitation. Our ultra-smooth surfaces are critical for implementing advanced optical solutions (e.g., total internal reflection lenses, solid immersion lenses, or waveguide coupling) suggested to reach the 50 pT/âHz shot-noise limit. |
| Microwave Delivery Structures | Custom Metalization Services: In-house deposition of Au, Pt, Pd, Ti, W, and Cu. | Necessary for fabricating the high-homogeneity microwave driving fields required for advanced pulsed schemes like Ramsey magnetometry, which offer significant sensitivity improvements over continuous wave methods. |
| Target Application | Engineering Support: Our in-house PhD team specializes in material selection and defect engineering for Quantum Sensing and Magnetocardiography (MCG) projects. | We provide consultation on optimizing nitrogen incorporation and subsequent irradiation/annealing protocols to achieve the required [NV-] concentration (4.6 ppm in this study) for ensemble sensing. |
For custom specifications or material consultation regarding high-sensitivity NV magnetometry, visit 6ccvd.com or contact our engineering team directly. We ship globally (DDU default, DDP available).
View Original Abstract
Nitrogen-vacancy centers (NVCs) in diamond are being explored for future quantum technologies, and in particular ensembles of NVC are the basis for sensitive magnetometers. We present a fiber-coupled NVC magnetometer with an unshielded sensitivity of (310±20)pT/âHz in the frequency range of 10-150 Hz at room temperature. This takes advantage of low-strain 12C diamond, lenses for fiber coupling and optimization of microwave modulation frequency, modulation amplitude, and power. Fiber coupling means the sensor can be conveniently brought within 2 mm of the object under study.