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Utilising NV based quantum sensing for velocimetry at the nanoscale

MetadataDetails
Publication Date2020-03-24
JournalScientific Reports
AuthorsD. Cohen, Ramil Nigmatullin, Oded Kenneth, Fedor Jelezko, Maxim Khodas
InstitutionsHebrew University of Jerusalem, Technion – Israel Institute of Technology
Citations20
AnalysisFull AI Review Included
  • Core Innovation: Development of a non-intrusive, nanoscale velocimetry technique utilizing Nitrogen-Vacancy (NV) centers in diamond for quantum sensing.
  • Mechanism: The NV centers measure the magnetic noise power spectrum (S(omega)) generated by the motion of unpolarized nuclear spins in the flowing liquid (nano-NMR spectroscopy).
  • Key Advantage (Diffusion Dominance): The method remains effective and highly sensitive even when diffusion noise is more dominant than the drift velocity noise, a major limitation for classic velocimetry techniques.
  • Performance Scaling: The scheme leverages the non-Lorentzian behavior of the power spectrum at low frequencies, achieving a sensitivity scaling proportional to the square root of the velocity (S proportional to 1 - square root(v)).
  • Sensitivity Improvement: Achieves an improvement of more than three orders of magnitude in fractional uncertainty compared to estimations based on the standard Lorentzian model, particularly for low-viscosity fluids like water.
  • Microfluidic Relevance: Provides crucial sensitivity to surface effects and flow profiles near boundaries, addressing the need for better understanding of flow characteristics in microfluidic and nanofluidic infrastructures.
  • Implementation: The technique relies only on statistical polarization, simplifying implementation compared to classic NMR velocimetry methods requiring strong, stable magnetic field gradients and efficient nuclear spin polarization.
ParameterValueUnitContext
NV Center Depth (d)5 to 15nmRange used for optimal sensitivity analysis (shallow NVs).
Water Nuclei Density (n)33nm-3Used in sensitivity calculations (equivalent to 3.3 x 1028 m-3).
Water Self-Diffusion Coefficient (D)2.3 x 103nm2/”sStandard experimental parameter (2.3 x 10-9 m2/s).
NV Ensemble Density (Upper Bound)1012cm-2Assumed density for ensemble sensitivity calculations.
Assumed Coherence Time (T2)100”sCoherence time assumed after dynamical decoupling.
BRMS (5 nm NV, Water)~250kHz/gammaeMagnetic field noise magnitude (gammae is the electron gyromagnetic ratio).
Dimensionless Velocity (v=1)150mm/sCorresponds to the drift velocity where the drift time scale equals the diffusion time scale (for water, d=15 nm).
Optimal Depth (Water, Intermediate Freq)15nmDepth where the power spectrum equals T2-1.
Fractional Velocity Uncertainty (Low Freq Regime, Ensemble)0.15 * square root(s / (T * V * A))DimensionlessAchieved sensitivity scaling, where T is total experiment time, V is velocity, and A is NV area.
MD Simulation Particle Count31,710ParticlesUsed the Lennard Jones (LJ) fluid model for verification.
  1. Quantum Sensor Setup: An ensemble of NV centers is located near the diamond surface, which forms the boundary of a microfluidic flow channel.
  2. Sensing Principle: The NV centers act as two-level systems whose relaxation rate (Gamma) is proportional to the power spectrum (S(omega)) of the magnetic noise generated by the nuclear spins in the flowing liquid.
  3. Measurement Protocols:
    • Decoherence Spectroscopy/Spin Relaxation: Measures the relaxation rate (Gamma) by optically probing the NV center population decay.
    • T0 Term Probing (Zero Frequency): Measures the classical noise term (related to thermal polarization fluctuations) via the NV’s pure dephasing time (T2).
    • T±1 Term Probing (Larmor Frequency): Measures the rotating noise term (used in nano-NMR) by introducing NV rotation at the Larmor frequency using pulsed dynamical decoupling sequences.
  4. Velocity Estimation Strategy:
    • Correlation Function Method: Preferred for highly viscous fluids (e.g., oil) or deeper NVs where the NV coherence time (T2) is shorter than the signal correlation time (tauD).
    • Power Spectrum Method: Preferred for low-viscosity fluids (e.g., water) and shallow NVs, utilizing the non-Lorentzian (square root) dependence on velocity at low frequencies for maximum sensitivity.
  5. Molecular Dynamics (MD) Simulation: A Lennard Jones (LJ) fluid model was used to simulate the dipole bath. The system was initialized thermally, and a constant drift velocity (v) was added. The z-component of the magnetic field Bz(t) at the NV position was computed over time to generate and fit the power spectra, validating the analytic scaling arguments.
  • Microfluidics and Nanofluidics: Essential for characterizing flow profiles, especially near channel boundaries, where the no-slip boundary condition may break down in nanoscale regimes.
  • Bio-medical Research (Lab-on-a-Chip): Provides high temporal and spatial resolution measurements required for advanced chemical and biological analysis platforms.
  • Quantum Sensing Technology: Advances the application of NV centers as nanoscale magnetometers and NMR spectrometers for complex dynamic systems.
  • Surface Science and Tribology: Enables non-intrusive investigation of fluid dynamics and boundary layer effects at solid-liquid interfaces.
  • High-Resolution Nano-NMR: Extends the capability of NV-based NMR to measure physical parameters (like velocity and diffusion coefficients) in minute liquid samples.