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Magnetic sensitivity enhancement via polarimetric excitation and detection of an ensemble of NV centers

MetadataDetails
Publication Date2024-05-23
JournalScientific Reports
AuthorsSimone Magaletti, Ludovic Mayer, Xuan Phuc Le, Thierry Debuisschert
InstitutionsThales (France)
Citations3
AnalysisFull AI Review Included

This research demonstrates a novel, easily implementable method to significantly enhance the magnetic sensitivity of Nitrogen-Vacancy (NV) center ensembles in diamond by leveraging polarization control.

  • Sensitivity Enhancement: Achieved an experimental improvement in magnetic sensitivity greater than a factor of two (up to 2.8x for specific families) compared to standard unpolarized detection setups.
  • Methodology: The enhancement is realized by tuning the polarization of the excitation laser (nL) using a half-wave plate (λ/2) and tuning the polarization of the detected Photoluminescence (PL) using a polarizer (nP).
  • Mechanism: Polarization tuning selectively maximizes the Optically Detected Magnetic Resonance (ODMR) contrast (C) of a single target NV center family while simultaneously minimizing the PL background (S0) emitted by the three non-participating families.
  • Contrast Achievement: The technique demonstrated a relative ODMR contrast of 60% for a single NV center family, which is 2.5 times higher than the expected baseline when all four families contribute equally.
  • Application Utility: This method is critical for improving the performance of vector magnetometers and for performing quantitative analysis of NV center preferential orientation distributions in diamond materials.
  • Simplicity: The proposed configuration requires only the addition of a half-wave plate and a polarizer to a standard NV center experimental setup.
ParameterValueUnitContext
NV Center TypeNegatively Charged (NV-)-Spin-1 color center in diamond
Ground State Zero-Field Splitting (D)2.87GHzResonance frequency at B=0
Gyromagnetic Ratio (γ)28GHz·T-1Used for magnetic field calculation
Excitation Wavelength532nmLinearly polarized laser source
PL Zero-Phonon Line (ZPL)637nmNV center radiative transition
PL Emission BandUp to 800nmBroad electron-phonon band
PL Filter Bandpass695/75nmSpectral filtering to suppress background noise
Objective Numerical Aperture (NA)0.28-PL collection system
Diamond Refractive Index (n1)2.4-Used for solid angle calculation
PL Collection Solid Angle (Ξ2)7°Calculated based on NA and n1
Maximum Relative Contrast (Simulated)0.63-Achieved by polarization optimization (2.5x baseline)
Maximum Sensitivity Enhancement (Simulated)2.4FactorRatio of optimized sensitivity parameter (χi) to baseline
Maximum Sensitivity Enhancement (Measured)2.8FactorMeasured improvement for Family D contrast parameter (ρD)

The experiment utilized a standard ODMR setup augmented with polarization control elements to selectively enhance the signal from a single NV center family.

  1. Sample and RF Setup: A CVD diamond crystal (Element Six) hosting NV center ensembles was glued onto a Coplanar Waveguide (CPW). The CPW delivered a linearly polarized RF magnetic field along the diamond (100) direction to ensure equal excitation of all four NV center families.
  2. Static Field Application: A Neodymium magnet was used to apply a static magnetic field, lifting the degeneracy of the |±1> spin sublevels and creating eight distinct ODMR peaks (two per NV family).
  3. Excitation Control: A 532 nm laser was directed through a half-wave plate (λ/2) to precisely control the laser polarization (nL) before exciting the NV centers through a {110} plane.
  4. Detection Control: PL was collected from a {100} lateral facet using a microscope objective (NA 0.28), filtered (695/75 nm), and passed through a polarizer (nP) before being detected by a CMOS camera.
  5. Polarizer Optimization (Step 1): The laser polarization (nL) was initially fixed along the (100) direction to ensure equal excitation. The polarizer axis (nP) was then rotated in the {100} plane to find the optimal angle that maximized the relative ODMR contrast (Ri) for the target NV families (A, B, C, D).
  6. Laser Polarization Optimization (Step 2): The polarizer axis (nP) was fixed at the angle determined in Step 1 (maximizing contrast for families B and D). The half-wave plate was then rotated to tune the laser polarization (nL) in the {110} plane, allowing for the suppression of PL contribution from non-target families.
  7. Sensitivity Quantification: The ODMR spectra were fitted to extract the contrast (Ci) and detected PL (S0). The sensitivity parameter (χi) was calculated based on the ratio Ci / √S0 to quantify the polarization-induced enhancement.

This polarization-based sensitivity enhancement technique has direct implications for high-performance quantum sensing and material characterization.

  • High-Sensitivity Magnetometry: Enables the development of more sensitive room-temperature magnetometers based on NV ensembles, crucial for applications requiring pT·Hz-1/2 sensitivity levels.
  • Vector Magnetic Field Sensing: Improves the signal-to-noise ratio for individual NV families, which is essential for accurate vector measurement of static magnetic fields using the inherent tetrahedral symmetry of the NV centers.
  • Quantum Diamond Microscopy: Enhances the contrast and signal quality in widefield magnetic imaging systems, leading to improved spatial resolution and detection limits for magnetic field mapping.
  • Diamond Material Characterization: Provides a robust, all-optical method for quantitative analysis of NV center preferential orientation distributions in synthetic diamond crystals (e.g., those grown along (110) or (113) directions), which is vital for optimizing quantum material quality.
  • Quantum RF Signal Analysis: Applicable to quantum radio frequency signal analyzers and detectors that rely on high-contrast ODMR measurements.
View Original Abstract

Abstract The negatively charged nitrogen-vacancy center (NV) presents remarkable spin-dependent optical properties that make it an interesting tool for magnetic field sensing. In this paper we exploit the polarization properties of the NV center absorption and emission processes to improve the magnetic sensitivity of an ensemble of NV centers. By simply equipping the experimental set-up of a half-wave plate in the excitation path and a polarizer in the detection path we demonstrate an improvement larger than a factor of two on the NV center magnetic sensitivity.