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Quantum magnetometer based on cross-relaxation resonances in ensembles of NV-centers in diamond

MetadataDetails
Publication Date2022-01-01
JournalЖурнал технической физики
AuthorsР. А. Ахмеджанов, Л. А. Гущин, I. V. Zelensky, Kupaev A.V., В. А. Низов
InstitutionsInstitute of Applied Physics
AnalysisFull AI Review Included

This research details the development and characterization of a novel quantum magnetometer based on Nitrogen-Vacancy (NV) centers in diamond, utilizing cross-relaxation (CR) resonances.

  • MW-Free Operation: The core innovation is the elimination of microwave (MW) radiation, a requirement for traditional optically detected magnetic resonance (ODMR) schemes, significantly broadening the applicability of the sensor.
  • Demonstrated Sensitivity: A magnetic field sensitivity of 18 nT/Hz1/2 was achieved in the scalar measurement regime using a 300 µm diamond crystal sensor.
  • Performance Metrics: The achieved sensitivity is only 1.7 times inferior to the calculated maximum theoretical shot-noise limit (10.7 nT/Hz1/2) for the current optical setup.
  • Sensor Material: The sensor utilizes a synthetic HPHT diamond crystal, electron-irradiated (1018 electrons per cm2) and annealed at 800 °C to create a high concentration of NV-centers.
  • Detection Method: High-accuracy measurements are enabled by a balanced photodetector scheme and lock-in detection operating optimally at 0.75 kHz.
  • Measurement Capability: The system supports both scalar (single projection) and vector (all projections) magnetic field measurements via an iterative procedure tracking the shift of CR resonances.
ParameterValueUnitContext
Achieved Sensitivity (Scalar)18nT/Hz1/2Average noise at frequencies > 0.6 Hz
Shot Noise Limit (Theoretical)10.7nT/Hz1/2Maximum possible sensitivity for the setup
Sensor MaterialSynthetic HPHTDiamondElectron irradiated
Sensor Size (Crystal)~300µmUsed for the working model
NV-Center Irradiation Dose1018electrons per cm2Post-growth treatment intensity
Annealing Temperature800°CPost-irradiation treatment
Laser Wavelength (Preferred)532nmCobolt 06-91 laser source
Optical Fiber Core Diameter200µmUsed for coupling light to the sensor
Numerical Aperture (NA)0.5-Optical fiber specification
Operating Pump Intensity50W/cm2Limited by adhesive layer thermal stability
Optimal Pump Intensity (Contrast)~100W/cm2Intensity maximizing CR resonance contrast
Lock-in Detection Frequency (Optimal)0.75kHzAlternating magnetic field component
Lock-in Detection Amplitude (Optimal)0.16mTAlternating magnetic field component
CR Resonance Measurement Range±200µTRange for each projection in vector regime

The magnetometer model relies on precise material engineering, optical alignment, and sophisticated electronic control:

  1. NV-Center Creation: A synthetic HPHT diamond crystal was selected, irradiated with an electron beam at 1018 electrons per cm2, and subsequently annealed at 800 °C to generate a high concentration of NV-centers.
  2. Sensor Assembly: The 300 µm diamond crystal was glued (using NOA63 optical adhesive) to the end face of a 200 µm core optical fiber (NA 0.5), ensuring the fiber axis aligned approximately with the diamond’s major crystallographic Z-axis ([0, 0, 1]).
  3. Optical Pumping: A 532 nm laser (Cobolt 06-91) was used for optical pumping. The operating intensity was limited to 50 W/cm2 to prevent overheating and destruction of the adhesive layer.
  4. Fluorescence Detection: Fluorescence was collected via the same fiber and routed to a PDB450A balanced photodetector. This balanced detection scheme was critical for suppressing residual noise from the laser intensity.
  5. Magnetic Field Control: A magnetic system consisting of a solenoid (scanning field) and two micro-coils (bias field) was used to apply and adjust the magnetic environment, enabling the tuning of the cross-relaxation resonance conditions.
  6. Lock-in Detection: An alternating magnetic field component (0.75 kHz, 0.16 mT) was applied to the solenoid. The sensor signal was processed using a custom FPGA board and Raspberry Pi 4 microcomputer to perform synchronous lock-in detection, maximizing the signal-to-noise ratio.
  7. Field Measurement: Magnetic field determination was achieved using an iterative procedure that measures the shift of the CR resonance centers (where the lock-in signal is zero). This procedure allows for both scalar and vector field determination.

The development of a compact, MW-free, high-sensitivity NV-center magnetometer opens doors for applications previously limited by the need for bulky microwave components or interference concerns.

  • Biomedical Imaging and Research: Ideal for magnetometry in biological environments (e.g., in-vivo sensing, magnetocardiography) where MW radiation is undesirable or near conductive tissues that shield RF signals.
  • Microscopic Magnetic Sensing: Enables the creation of highly localized, non-invasive probes for measuring magnetic fields in integrated circuits, materials science samples, or small-scale devices.
  • Industrial Non-Destructive Testing (NDT): Use in detecting magnetic anomalies or defects in materials without requiring complex RF shielding or large external coils.
  • Compact Quantum Sensors: Provides a pathway for developing robust, small-form-factor quantum magnetometers for field use, navigation, or defense applications where size, weight, and power (SWaP) are critical constraints.
  • High-Frequency Magnetic Field Measurement: The demonstrated operational frequency range (0.5-10 kHz) is suitable for measuring dynamic magnetic phenomena.
View Original Abstract

We create a working model of a magnetometer of a new type that is based on using cross-relaxation resonances in ensembles of NV-centers in diamond. This type of magnetometer does not require microwave radiation. For a sensor made out of a 300 micron diamond we demonstrate the magnetic field sensitivity of around 18 nT/Hz 1/2 . Keywords: cross-relaxation, NV-center, quantum magnetometer.