Skip to content

Spin coherence and depths of single nitrogen-vacancy centers created by ion implantation into diamond via screening masks

MetadataDetails
Publication Date2020-06-24
JournalJournal of Applied Physics
AuthorsShuntaro Ishizu, Kento Sasaki, Daiki Misonou, Tokuyuki Teraji, Kohei M. Itoh
InstitutionsKeio University, RIKEN Center for Emergent Matter Science
Citations6
AnalysisFull AI Review Included

This research characterizes single Nitrogen-Vacancy (NV) centers created near the diamond surface using a novel ion implantation technique, focusing on the relationship between NV depth (dNV) and spin coherence time (T2).

  • Novel Implantation Method: Near-surface NV centers were successfully created using a comparatively high energy (10 keV) N+ ion implantation combined with a thin Silicon Dioxide (SiO2) screening mask.
  • Depth Profile Validation: The resulting NV depth profile was concentrated toward the surface (unlike standard Gaussian profiles), with a large portion of centers located within 10 nm, consistent with Monte Carlo (SRIM) simulations.
  • Coherence-Depth Correlation: A clear trend was established: deeper NV centers exhibit longer T2,echo. The measured T2,echo vs. dNV relation is comparable to results from other low-energy implantation methods.
  • Yield and Density: The conversion efficiency (yield) from implanted N+ ions to active NV centers was low (0.1-0.4%), similar to standard low-energy implantation results.
  • Noise Limitation: Noise spectroscopy confirmed that magnetic noise, likely originating from paramagnetic surface defects, is the dominant factor limiting the spin coherence time (T2) in these near-surface NV centers.
  • Surface Instability: The T2 of shallow NV centers was observed to be unstable or degrade over time, a phenomenon potentially linked to slight morphological changes (wrinkles) observed on the diamond surface after the SiO2 deposition and processing steps.
ParameterValueUnitContext
Ion Implantation Species14N+N/AUsed instead of 15N+ due to use of 12C CVD layer
Ion Implantation Energy10keVRelatively high energy for near-surface creation
Ion Implantation Dose1011cm-2Target dose for single NV resolution
SiO2 Mask Thickness (t) Range52.3 to 69.1nmVaried to control implantation profile
NV Center Yield (Efficiency)0.1 - 0.4%Conversion efficiency from N+ to NV-
Maximum T2,echo Measured27.1”sAchieved using Hahn echo sequence
Shallowest dNV Measured14.4nmDetermined via proton NMR (XY16-128 sequence)
Magnetic Field (B0)23.2mTApplied parallel to NV axis for ODMR/NMR
Proton NMR Frequency (ωn/2π)0.988MHzCalculated value for 23.2 mT field
Magnetic Noise Rate (Ω)316HzDeduced from Single Quantum (SQ) relaxation
Electric Noise Rate (Îł)272HzDeduced from Double Quantum (DQ) relaxation
Surface Roughness (Rrms, t=0)0.11nmAFM measurement on blocked area
Surface Roughness (Rrms, t≠0)0.14nmAFM measurement on implanted area
Longest T2,drive Achieved43.0”sUnder N-pulse dynamical decoupling (N=512)

The creation and characterization of single NV centers involved precise material growth, implantation, and multi-stage annealing and cleaning processes:

  1. Substrate Selection: Began with a natural abundant (1.1% 13C) Type-IIa (001) diamond substrate.
  2. CVD Growth: An undoped, isotopically pure 12C layer (99.95%) was grown by Chemical Vapor Deposition (CVD) to a thickness of a few microns to suppress nuclear spin bath noise (13C).
  3. Screening Mask Deposition: SiO2 layers were deposited using electron beam evaporation. A metal plate with four apertures was used to create areas with controlled thicknesses (t = 52.3, 57.6, 64.1, and 69.1 nm).
  4. Ion Implantation: 14N+ ions were implanted at 10 keV energy with a dose of 1011 cm-2, passing through the deposited SiO2 screening masks.
  5. Mask Removal: The SiO2 layers were subsequently removed using hydrofluoric acid (HF).
  6. Annealing (Vacancy Diffusion): The sample was annealed at 800 °C for 2 hours in vacuum (9.7 x 10-7 torr) to promote vacancy diffusion and NV center formation.
  7. Annealing (Charge State Conversion): A second annealing step was performed at 450 °C for 9 hours in an oxygen atmosphere to convert neutral NV0 centers into the desired negatively charged NV- state.
  8. Chemical Cleaning: The sample underwent rigorous chemical cleaning using a triacid mixture (sulfuric, nitric, and perchloric acids) and a piranha solution (H2O2/sulfuric acid).
  9. Quantum Characterization: Single NV centers were measured using Optically Detected Magnetic Resonance (ODMR), Hahn Echo (T2,echo), Dynamical Decoupling (XYk sequences) for noise spectroscopy, and Proton Ensemble NMR for dNV determination.

The precise engineering of shallow NV centers is critical for applications requiring strong coupling between the quantum sensor and external analytes or fields.

  • Nano-scale NMR and MRI: The primary application is high-sensitivity Nuclear Magnetic Resonance (NMR) spectroscopy and imaging of analyte ensembles (e.g., proteins, chemicals) placed directly on the diamond surface, requiring NV centers within 5-10 nm of the surface.
  • Quantum Sensing and Magnetometry: Development of high-resolution quantum sensors for detecting magnetic and electric fields, particularly in environments where surface proximity is necessary (e.g., measuring current flow in 2D materials).
  • Quantum Communication and Photonics: Integration of shallow NV centers into nanophotonic and plasmonic structures to enhance light coupling efficiency, crucial for quantum network nodes and quantum light sources.
  • Diamond Material Processing: Provides a validated, high-energy implantation recipe combined with screening masks, offering an alternative to standard low-energy implantation for creating high-quality, shallow defect layers in CVD diamond.
  • Surface Science Research: The methodology provides a tool for investigating and characterizing surface defects and noise sources that limit quantum coherence, informing future surface passivation and cleaning protocols.
View Original Abstract

We characterize single nitrogen-vacancy (NV) centers created by 10-keVN+ ion implantation into diamond via thin SiO2 layers working as screening masks. Despite the relatively high acceleration energy compared with standard ones (<5keV) used to create near-surface NV centers, the screening masks modify the distribution of N+ ions to be peaked at the diamond surface [Ito et al., Appl. Phys. Lett. 110, 213105 (2017)]. We examine the relation between coherence times of the NV electronic spins and their depths, demonstrating that a large portion of NV centers are located within 10 nm from the surface, consistent with Monte Carlo simulations. The effect of the surface on the NV spin coherence time is evaluated through noise spectroscopy, surface topography, and x-ray photoelectron spectroscopy.

  1. 2013 - Nanoscale nuclear magnetic resonance with a nitrogen-vacancy spin sensor [Crossref]
  2. 2013 - Nuclear magnetic resonance spectroscopy on a (5-Nanometer)3 sample volume [Crossref]
  3. 2014 - Nuclear magnetic resonance spectroscopy with single spin sensitivity [Crossref]
  4. 2015 - Nanoscale nuclear magnetic imaging with chemical contrast [Crossref]
  5. 2015 - Nanoscale NMR spectroscopy and imaging of multiple nuclear species [Crossref]
  6. 2016 - Nuclear magnetic resonance detection and spectroscopy of single proteins using quantum logic [Crossref]
  7. 2017 - Nanoscale nuclear magnetic resonance with chemical resolution [Crossref]
  8. 2013 - Quantum plasmonics [Crossref]
  9. 2016 - Quantum nanophotonics in diamond [Crossref]
  10. 2018 - Material platforms for spin-based photonic quantum technologies [Crossref]