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TR12 centers in diamond as a room temperature atomic scale vector magnetometer

MetadataDetails
Publication Date2022-06-02
Journalnpj Quantum Information
AuthorsJonas Foglszinger, Andrej Denisenko, Thomas Kornher, M. Schreck, Wolfgang Knolle
InstitutionsUniversity of Augsburg, Centre National de la Recherche Scientifique
Citations13
AnalysisFull AI Review Included

TR12 Centers in Diamond: Room Temperature Vector Magnetometry

Section titled “TR12 Centers in Diamond: Room Temperature Vector Magnetometry”

TR12 defects in diamond are presented as a robust, room-temperature alternative to Nitrogen-Vacancy (NV) centers for atomic-scale magnetometry, specifically addressing limitations in high-field, arbitrary-orientation sensing.

  • Vector Magnetometry: TR12 centers enable full vector magnetometry under ambient conditions, unlike NV centers which are highly sensitive only along their symmetry axis.
  • High Field Tolerance: The defect maintains strong Optically Detected Magnetic Resonance (ODMR) contrast (up to 30%) even when exposed to strong, off-axis magnetic fields up to 1 T and beyond.
  • Spin Mechanism: The sensing relies on coherent control of a metastable excited triplet state (S=1) with long microsecond-range lifetimes (e.g., τx = 8.3 ”s, τy = 7.4 ”s).
  • Sensitivity: The estimated shot-noise limited magnetic sensitivity for a single TR12 center is 3.9 ”T Hz-1/2.
  • Defect Structure: TR12 exhibits twelve inequivalent orientations in the diamond lattice, ensuring that at least two orientations are always optimally aligned for vector sensing in bulk measurements.
  • Jahn-Teller Effect: The defect displays a static Jahn-Teller distortion, causing switching between two spatial configurations, which manifests as anomalous splitting of ODMR lines in an external magnetic field.
  • Fabrication: TR12 centers can be artificially created via standard methods (ion implantation or electron irradiation), facilitating integration into engineered diamond devices.
ParameterValueUnitContext
Operating TemperatureRoom°CAmbient conditions
Maximum Field Tolerance1 and beyondTMaintains contrast at high, arbitrary fields
Zero Phonon Line (ZPL)471nmOptical transition wavelength
Excitation Wavelength410nmLinear polarized laser
Zero-Field Splitting (D)1636.6MHzTriplet state (S=1)
Zero-Field Splitting (E)896.6MHzTriplet state (S=1)
Excited Singlet Lifetime (τS1)4.69nsEmitting state lifetime
Long-Lived Triplet Lifetime (τmeta)6.79”sOverall metastable decay (Tx and Ty combined)
Short-Lived Triplet Lifetime (τz)375nsFitted from Rabi oscillation decay
ODMR Contrast (Max)Up to 30%Observed in zero magnetic field
Shot-Noise Sensitivity (η)3.9 ”T Hz-1/2”T Hz-1/2Estimated for single center (1 MHz linewidth)
Magnetic Field Shift (CM)28GHz per TFrequency shift of ODMR resonance

The TR12 centers were created and characterized using standard diamond defect engineering and advanced confocal microscopy techniques.

  1. Substrate Preparation: Experiments utilized Chemical Vapor Deposition (CVD) diamond samples oriented along the (100) plane.
  2. Defect Creation (Option 1: Ion Implantation): TR12 centers were created using 12C ion implantation at energies of 10 keV or 370 keV, with a dose of 1011 ions per cm2.
  3. Defect Creation (Option 2: Electron Irradiation): Alternatively, defects were created using 10 MeV electron irradiation at a dose of 5 x 1016 e per cm2.
  4. Thermal Processing: All samples underwent post-irradiation/implantation annealing at 800 °C for 1 hour to activate the defects.
  5. Optical Characterization: A home-built confocal microscope was used for spectroscopic studies, employing a 410 nm linear polarized laser for excitation.
  6. Microwave Delivery: Spin control was achieved using microwave radiation supplied to the sample via a lithographically defined golden microwave waveguide placed on the diamond surface.
  7. Magnetic Field Control: A permanent magnet (NdFeB, 1.4 T magnetization) was positioned above the sample using high-precision stepper motors, allowing for continuous variation of the magnetic field magnitude and orientation relative to the defect.

The unique properties of TR12 centers—room-temperature operation, high-field tolerance, and vector sensing capability—make them highly relevant for several high-tech sectors.

  • Quantum Sensing and Metrology:
    • Nanoscale Vector Magnetometry: Enabling full 3D magnetic field mapping with nanoscale spatial resolution in complex environments where field orientation is arbitrary.
    • High-Field Calibration: Precise calibration and monitoring of strong magnetic fields, such as those used in advanced Magnetic Resonance Imaging (MRI) scanners or high-power industrial equipment.
    • Strain and Temperature Sensing: Potential for sensing local strain and temperature at the nanoscale, though responsivity requires further assessment.
  • Solid-State Quantum Information Processing (QIP):
    • Nuclear Spin Readout: Utilizing the triplet state for initializing and reading out nearby nuclear spin qubits (e.g., 13C), potentially offering longer nuclear memory lifetimes due to the spin-free ground state.
    • Quantum Interfaces: Serving as a robust quantum interface between stationary qubits (nuclear spins) and flying qubits (photons) when integrated into photonic crystal microcavities (Purcell enhancement).
  • Advanced Materials and Defect Engineering:
    • Diamond Electronics: Expanding the family of robust, optically active spin defects available for integration into diamond-based quantum devices and sensors.
    • Fundamental Physics: Studying complex electronic-vibrational coupling phenomena, such as the static Jahn-Teller effect, in a solid-state host.