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Subnanotesla Magnetometry with a Fiber-Coupled Diamond Sensor

MetadataDetails
Publication Date2020-10-30
JournalPhysical Review Applied
AuthorsR. L. Patel, Li Zhou, Angelo Frangeskou, G. A. Stimpson, Ben G. Breeze
InstitutionsEngineering and Physical Sciences Research Council, Element Six (United Kingdom)
Citations62
AnalysisFull AI Review Included

This analysis summarizes the development and performance of a highly sensitive, fiber-coupled diamond magnetometer designed for portable applications like magnetocardiography (MCG).

  • Core Achievement: Demonstrated sub-nanotesla (sub-nT) sensitivity, achieving (310 ± 20) pT/√Hz in the 10-150 Hz frequency range using applied test fields.
  • Technology: Optically Detected Magnetic Resonance (ODMR) utilizing an ensemble of Nitrogen Vacancy (NV) centers in a high-purity, 12C-enriched CVD diamond.
  • Key Innovation: Integration of aspheric lenses within the sensor head to efficiently couple excitation light into the diamond and collect fluorescence back into the fiber, significantly reducing optical losses.
  • Portability: The fiber-coupled design separates the bulky control instrumentation (lasers, microwaves) from the sensor head, allowing the sensor to be placed conveniently within 2 mm of the object under study.
  • Performance Context: This sensitivity represents a significant improvement over previous fiber-coupled NV magnetometers (35 nT/√Hz using applied fields) and is a factor of ~6 away from the estimated photon shot-noise limit (50 pT/√Hz).
  • Future Outlook: Achieving the sensitivity required for MCG (estimated to be an order of magnitude better) will require improvements in photon collection efficiency (currently 0.03%) and implementation of noise cancellation techniques (e.g., gradiometry or dual-resonance methods).
ParameterValueUnitContext
Achieved Sensitivity310 ± 20pT/√HzMeasured using applied test fields (10-150 Hz)
Photon Shot Noise Limit50pT/√HzCalculated theoretical limit
Zero-Field Splitting (D)~2.87GHzNV ground state at room temperature
Hyperfine Splitting (A)~2.16MHzInteraction with 14N nuclear spin
Optimal Microwave Power~0.8WApplied power after amplification
Optimal Modulation Frequency3.0307kHzFrequency modulation rate
Optimal Frequency Depth300kHzFrequency modulation deviation
Laser Wavelength532nmExcitation source (Laser Quantum Gem-532)
Laser Power Used1WUsed to reduce laser noise
Excitation Fiber Core Diameter400”mThorlabs FG400AEA fiber
Diamond Dimensions4 x 4 x 0.6mmSingle crystal sample size
Diamond Orientation(100)-Crystallographic orientation
Diamond Isotope Purity99.995%12CCarbon enrichment
NV- Concentration4.6ppmNegatively charged NV concentration
Fluorescence Collection Efficiency0.03%Calculated conversion efficiency (Green to Red)
Diamond Refractive Index (nd)2.42-Limits light collection due to TIR
Measured Linewidth (ΔΜ)1.11MHzExtracted from ODMR spectrum
Measured Contrast (C)1.76%Extracted from ODMR spectrum

The magnetometry system relies on continuous wave (CW) ODMR using a fiber-coupled setup optimized for high photon collection efficiency.

  1. Excitation and Noise Reduction: A 532 nm laser (1 W) is used for excitation. Approximately 1% of the beam is sampled and fed to a balanced detector (Thorlabs PDB450A) reference arm to actively cancel out laser intensity noise.
  2. Fiber Coupling and Focusing: The main laser beam is coupled into a 400 ”m core fiber. The fiber output is collimated by the first aspheric lens (C171TMD-B) and focused onto the diamond by the second lens (C330TMD-B). These same lenses collect the resulting NV fluorescence.
  3. Microwave Delivery: Microwaves (2-4 GHz) are generated, amplified (Mini-Circuits ZHL-16W-43-S+), and delivered via a coaxial circulator to a 5 mm copper loop antenna deposited on an aluminum prototyping board, which also serves for heat management.
  4. Magnetic Field Alignment: A permanent rare earth magnet is aligned to the (111) crystallographic axis of the NV ensemble to provide the necessary Zeeman splitting.
  5. Signal Detection and Modulation: The balanced detector output is fed to a lock-in amplifier (Zurich MFLI). The microwave frequency is square-wave modulated, and a 2.158 MHz sinewave is mixed in to utilize hyperfine excitation for improved contrast.
  6. Optimization: Sensitivity was optimized by systematically varying the microwave power (0.06 W to 3.16 W pre-amplification), frequency modulation depth (100 kHz to 600 kHz), and modulation frequency (1 kHz to 80 kHz) to maximize the zero-crossing slope of the derivative spectrum.
  7. Sensitivity Measurement: Sensitivity was determined using two methods: (1) calculating the zero-crossing slope (yielding 171 pT/√Hz) and (2) applying calibrated test fields via a Helmholtz coil along the (100) direction (yielding 310 ± 20 pT/√Hz).

The combination of sub-nT sensitivity and high portability makes this fiber-coupled NV diamond sensor suitable for several advanced engineering and medical applications:

  • Medical Diagnostics (MCG): The primary target application is Magnetocardiography (MCG), requiring highly sensitive, non-invasive magnetic field detection near the body. The compact, mobile sensor head is ideal for clinical settings.
  • Geology and Materials Inspection: Sensing small magnetic fields for geological surveys or non-destructive testing of materials where the sensor must be brought into close proximity (less than 2 mm) to the sample.
  • Portable Quantum Sensing: Development of robust, field-deployable quantum sensors that require high sensitivity without the need for cryogenic cooling (room temperature operation).
  • Compact Instrumentation: Integration into complex systems where the control electronics must be physically separated from the sensing element, such as in boreholes, confined spaces, or integrated circuit testing.
  • Temperature-Invariant Sensing: Future implementation of dual-resonance or double-quantum magnetometry techniques will enable highly stable, temperature-invariant sensors crucial for industrial monitoring and field use.
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/√Hz 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.