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Room Temperature Electrically Detected Nuclear Spin Coherence of NV Centres in Diamond

MetadataDetails
Publication Date2020-01-21
JournalScientific Reports
AuthorsHiroki Morishita, S. Kobayashi, Masanori Fujiwara, Hiromitsu Kato, Toshiharu Makino
InstitutionsKyoto University, Japan Science and Technology Agency
Citations28
AnalysisFull AI Review Included

This research demonstrates the successful electrical detection of nuclear spin coherence in Nitrogen-Vacancy (NV) centers in diamond at room temperature, a critical step toward integrated quantum devices.

  • Core Achievement: First demonstration of room-temperature electrical detection of 14N nuclear spin coherence in NV centers using the Electrically Detected Electron-Nuclear Double Resonance (EDENDOR) technique.
  • Coherence Time: A nuclear spin coherence time (T2(n)) of approximately 0.9 ms was measured at 300 K.
  • Limitation: The measured T2(n) is currently limited by the longitudinal relaxation time of the NV electron spins (T1(e) ≈ 1.8 ms).
  • Detection Mechanism: The EDENDOR signal is observed as a change in the photocurrent (ΔQ) generated via two-photon ionization by a 532 nm laser.
  • Sensitivity Advantage: Electrical detection of electron spin coherence is theoretically predicted to offer approximately three times higher sensitivity than traditional optical techniques.
  • Material System: Ensemble NV centers were created in a highly P-doped n-type diamond layer (P-donor concentration ~1018 cm-3) to ensure high electrical conductivity.
  • Future Impact: The results pave the way for developing novel, all-electrical, integrated electron- and nuclear-spin-based diamond quantum memories and sensors.
ParameterValueUnitContext
Nuclear Spin Coherence Time (T2(n))0.9 (±0.5)msMeasured at room temperature (lower limit).
Electron Spin Relaxation Time (T1(e))1.8 (±0.6)msMeasured via EDMR technique.
14N Nuclear Spin Resonance Frequency3.5MHzEDENDOR signal frequency (transition:
NV Electron Rabi Oscillation Frequency~4.4MHzMeasured with 5 W MW input power.
Laser Wavelength532nmUsed for initialization and two-photon ionization.
Laser Power (Photocurrent Generation)30mWUsed for pEDMR/pODMR measurements.
Static Magnetic Field (B0)~10GApplied approximately along the [111] direction.
Applied Voltage (Photocurrent Detection)8VConstant voltage applied across interdigital contacts.
P-donor Concentration (n-type layer)~1018cm-3Doping concentration of the CVD-grown diamond layer.
NV Center Concentration (Estimated)1 x 1015cm-3Concentration within the detection volume.
N+-ion Implantation Dose1 x 1015cm-2Used for creating NV centers.
N+-ion Kinetic Energy350keVUsed for creating NV centers.
Diamond Layer Thickness10”mThickness of the P-doped n-type layer.
Interdigital Contact Gap~2”mGap size between electrical contacts.

The experiment utilized a self-built EDENDOR spectrometer and specially prepared P-doped n-type diamond samples.

  1. Substrate: Type IIa (001) diamond substrate.
  2. Growth: A 10 ”m thick P-doped n-type diamond layer was synthesized via Chemical Vapour Deposition (CVD), achieving a P-donor concentration of ~1018 cm-3.
  3. NV Creation: Ensemble NV centers were created via 14N+-ion implantation (350 keV kinetic energy, 1 x 1015 cm-2 dose).
  4. Annealing: The sample was annealed at 1000 °C for 1 hour under vacuum.
  5. Contact Fabrication: Interdigital contacts with ~2 ”m gaps were fabricated using electron-beam lithography.
  6. Metallization: Ti(30 nm)/Pt(30 nm)/Au(100 nm) multi-layers were deposited, followed by annealing at 420 °C in an Argon atmosphere.

The EDENDOR technique was implemented using a pulsed sequence to measure Rabi oscillations and T2(n).

  1. Initialization: NV electron spins are initialized to the |0> state using a pulsed 532 nm laser.
  2. Manipulation: Electron spins are manipulated using Microwave (MW) pulses (e.g., π-pulse at 2916 MHz). Nuclear spins are manipulated using Radio-Frequency (RF) pulses (e.g., 3.5 MHz).
  3. Photocurrent Generation: A final 532 nm laser pulse generates a photocurrent via two-photon ionization.
  4. Detection: The change in photocurrent (ΔQ) is measured by integrating the transient current (ΔI) over time, using a current amplifier and digitizer under a constant 8 V bias.
  5. T2(n) Measurement: A modified EDENDOR sequence incorporating a nuclear-spin Hahn echo sequence was used to measure the T2(n) decay as a function of the free evolution time (2τ).
  6. Noise Mitigation: A phase cycling technique was applied to subtract artifact noises arising from off-resonant MW/RF contributions and laser-power fluctuations.

This technology is foundational for developing next-generation quantum hardware, particularly where room-temperature operation and integration are critical.

  • Quantum Computing and Memory:

    • Quantum Registers: Utilizing the NV electron spin for fast manipulation and the 14N nuclear spin for long-term, robust quantum memory (T2(n) ≈ 0.9 ms at 300 K).
    • Integrated Qubits: Enabling the fabrication of all-electrical quantum devices that can be integrated into standard semiconductor architectures, eliminating the need for complex, bulky optical readout systems.
  • Quantum Sensing:

    • Highly Sensitive Magnetometers: Developing room-temperature, highly sensitive magnetic sensors based on NV centers, leveraging the enhanced sensitivity of electrical detection.
    • Nanoscale Spectroscopy: Using nuclear spin memory to enable sensor-unlimited nanoscale spectroscopy of small spin clusters.
  • Diamond Electronics:

    • High-Conductivity Platforms: The use of highly P-doped n-type diamond provides a robust, electrically conductive platform necessary for efficient current detection and integration of quantum components.
    • Hybrid Devices: Development of hybrid solid-state devices combining classical diamond electronics with quantum spin functionalities.
View Original Abstract

Abstract We demonstrate electrical detection of the 14 N nuclear spin coherence of NV centres at room temperature. Nuclear spins are candidates for quantum memories in quantum-information devices and quantum sensors, and hence the electrical detection of nuclear spin coherence is essential to develop and integrate such quantum devices. In the present study, we used a pulsed electrically detected electron-nuclear double resonance technique to measure the Rabi oscillations and coherence time ( T 2 ) of 14 N nuclear spins in NV centres at room temperature. We observed T 2 ≈ 0.9 ms at room temperature, however, this result should be taken as a lower limit due to limitations in the longitudinal relaxation time of the NV electron spins. Our results will pave the way for the development of novel electron- and nuclear-spin-based diamond quantum devices.