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Polarization Transfer to External Nuclear Spins Using Ensembles of Nitrogen-Vacancy Centers

MetadataDetails
Publication Date2021-05-24
JournalPhysical Review Applied
AuthorsA. J. Healey, L. T. Hall, G.A.L. White, T. Teraji, Sani Ma
InstitutionsNational Institute for Materials Science, Centre for Quantum Computation and Communication Technology
Citations27
AnalysisFull AI Review Included

This study experimentally validates the feasibility of using dense, shallow Nitrogen-Vacancy (NV) center ensembles in diamond to hyperpolarize external nuclear spins, aiming to significantly enhance Nuclear Magnetic Resonance (NMR) sensitivity.

  • Scalability Demonstrated: Polarization transfer was successfully achieved from a dense NV ensemble (addressing ~106 NVs in parallel) to external hydrogen targets over a 50x50 ”m field of view, scaling up previous single-NV results.
  • Maximum Transfer Rate: A peak polarization transfer rate of ~7500 spins per second per NV was measured for a solid biphenyl target, confirming sufficient coupling strength in current “best case” shallow ensembles.
  • Protocol Robustness: The PulsePol sequence was utilized, demonstrating robustness against broadband noise inherent to dense, near-surface NV ensembles, achieving NV coherence times (T2) in excess of 10 ”s.
  • Liquid Target Feasibility: Polarization transfer efficiency to sufficiently viscous liquid targets (glycerol) was only reduced by a factor of 2-3 compared to solids, suggesting NV-based liquid-state hyperpolarization is viable, especially if surface effects reduce molecular diffusion near the diamond.
  • Material Limitations Identified: Current NV yield (1.4%) and coherence degradation due to surface defects and nitrogen spin bath limit the steady-state polarization enhancement to three orders of magnitude over Boltzmann levels.
  • Future Enhancement Potential: The authors estimate that realistic improvements in diamond material quality (especially surface control and NV yield) could lead to a total enhancement of up to two orders of magnitude beyond current results, making the technique competitive for NMR enhancement.
ParameterValueUnitContext
Diamond SubstrateElectronic Grade CVDN/AIsotopically enriched (99.95% 12C)
12C Layer Thickness1”mOvergrown layer
Implant Species/Energy15N2.5 keVUsed to create shallow NVs
Implant Fluence (D1)1 x 1013cm-2Sample D1
Implant Fluence (D2)2 x 1013cm-2Sample D2 (higher N density)
Annealing Temperature1100°CRamped anneal
Mean NV Depth (dNV)~6nmMeasured via XY8-k spectroscopy
Areal NV Density (σNV)~1500”m-2Estimated average density
NV Yield (D1 / D2)1.4% / 0.9%N/AOverall N to NV conversion ratio
NV Coherence Time (TNV)~22”sD1, off-resonance PulsePol decay
PulsePol Coherence Time (T2)> 10”sAchieved using the decoupling sequence
Maximum Cooling Rate (u)~7500spins/s per NVMeasured for biphenyl solid target
Steady-State Polarization (P)2.7 x 10-4N/APredicted in 1 ”m layer (3 orders enhancement)
External Bias Field (B)~450GLow magnetic field operation
Laser Wavelength532nmNV excitation and initialization
Laser Incident Intensity~300mWUsed for widefield NV microscope
Target Diffusion (Biphenyl, Dn)~571nm2/sEstimated value for solid target
Target T1,n (Fit)~0.88sFitted value for biphenyl polarization buildup
  1. Diamond Substrate Preparation: Electronic grade CVD diamond substrates were used, featuring a 1 ”m thick layer of isotopically enriched 12C (99.95%) to minimize spin noise from the carbon lattice.
  2. Shallow NV Ensemble Creation: NVs were created using low-energy (2.5 keV) 15N ion implantation (fluence 1-2 x 1013 cm-2), followed by a high-temperature ramped anneal (up to 1100 °C) to activate the NVs.
  3. Surface Termination: The diamond surface was cleaned and oxygen-terminated using a boiling mixture of sulfuric and nitric acid to ensure a clean, stable surface environment.
  4. Target Deposition: Solid targets (biphenyl, PMMA) and liquid targets (glycerol/water mixtures, viscous oil) were deposited directly onto the diamond surface. Biphenyl crystals were formed by drying an isopropanol solution and then encapsulated in UV-curing epoxy.
  5. Widefield NV Microscopy: Experiments were conducted using a custom widefield NV microscope setup, allowing simultaneous addressing and readout of ~106 NVs over a 50x50 ”m field of view using a 532 nm laser and sCMOS camera.
  6. PulsePol Protocol Implementation: The robust PulsePol sequence, a Hamiltonian engineering protocol, was delivered via a gold ring-shaped microwave resonator to achieve resonant flip-flop coupling between the NV electron spins and the external nuclear spins (hydrogen).
  7. Polarization Measurement: Polarization transfer efficiency was inferred by measuring the normalized NV photoluminescence (PL) decay difference between resonant (on-resonance) and non-resonant (off-resonance) PulsePol sequences. The NV depolarisation rate was used as a proxy for the hydrogen cooling rate.

This research directly supports the development of next-generation hyperpolarization technology, primarily targeting enhanced sensitivity in NMR and related quantum sensing fields.

  • NMR Sensitivity Enhancement: The core application is improving the sensitivity of conventional bulk NMR by using the NV ensemble as a room-temperature, low-field hyperpolarizer, potentially replacing complex cryogenic Dynamic Nuclear Polarization (DNP) systems.
  • Micron-Scale NMR (NV-NMR): Enables high-resolution NMR spectroscopy and imaging of extremely small liquid or solid samples (picoliter volumes), crucial for microfluidics, chemical analysis, and biological studies where sample volume is limited.
  • Quantum Sensing Platforms: The methodology validates the use of dense, shallow NV ensembles for external spin manipulation, a key requirement for advanced quantum magnetometry and spectroscopy applications.
  • High-Purity Diamond Materials: Drives demand for high-quality, electronic-grade CVD diamond substrates with precise isotopic enrichment (12C) and optimized low-energy ion implantation recipes for creating stable, shallow NV layers.
  • Pharmaceutical and Chemical Analysis: Enhanced NMR sensitivity allows for faster analysis of low-concentration compounds or small samples, accelerating drug discovery and chemical reaction monitoring.
View Original Abstract

The nitrogen-vacancy (N-V) center in diamond has emerged as a candidate to noninvasively hyperpolarize nuclear spins in molecular systems to improve the sensitivity of nuclear magnetic resonance (NMR) experiments. Several promising proof-of-principle experiments have demonstrated small-scale polarization transfer from single N-V centers to hydrogen spins outside the diamond. However, the scaling up of these results to the use of a dense N-V ensemble, which is a necessary prerequisite for achieving realistic NMR sensitivity enhancement, has not yet been demonstrated. In this work, we present evidence for a polarizing interaction between a shallow N-V ensemble and external nuclear targets over a micrometer scale, and characterize the challenges in achieving useful polarization enhancement. In the most favorable example of the interaction with hydrogen in a solid-state target, a maximum polarization transfer rate of approximately 7500 spins per second per N-V is measured, averaged over an area containing order 106 N-V centers. Reduced levels of polarization efficiency are found for liquid-state targets, where molecular diffusion limits the transfer. Through analysis via a theoretical model, we find that our results suggest that implementation of this technique for NMR sensitivity enhancement is feasible following realistic diamond material improvements.