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Coherent electrical control of single electron spin in diamond nitrogen-vacancy center

MetadataDetails
Publication Date2022-01-01
JournalActa Physica Sinica
AuthorsJiandong Wu, Cheng Zhi, Xiangyu Ye, Zhaokai Li, Pengfei Wang
AnalysisFull AI Review Included

This research demonstrates the successful implementation of coherent electrical control (E-field) over the electron spin of a Nitrogen-Vacancy (NV) center in diamond, a critical step for integrating quantum systems with classical electronics.

  • Core Achievement: Coherent electrical driving of the NV electron spin, resulting in Electrically Driven Rabi Oscillations (ERabi) between the magnetic-dipole forbidden |ms = -1> and |ms = +1> states (a Delta ms = ±2 transition).
  • Control Mechanism: The transverse alternating electric field (E⊄) directly couples to the spin states, bypassing the need for complex, bulky magnetic field coils for this specific transition.
  • Scaling Law: The ERabi oscillation frequency is confirmed to be linearly proportional to the square root of the applied E-field power (fERabi āˆ √W), demonstrating predictable and tunable control speed.
  • Full Spin Manipulation: By combining the E-field control (for Delta ms = ±2 transitions) with conventional magnetic control (for Delta ms = ±1 transitions), full, direct coherent control over all three ground-state spin levels (|0>, |+1>, |-1>) is achieved.
  • Integration Potential: E-field control utilizes micro-fabricated electrodes, making it highly compatible with semiconductor chips and integrated quantum devices, overcoming the localization and shielding challenges inherent to magnetic control.
  • Performance Metric: A Ļ€-pulse duration of 6.65 µs was achieved at 0.28 W power, allowing for hundreds of quantum logic gate operations within the measured 1.6 ms coherence time (T2).
ParameterValueUnitContext
Diamond MaterialCVD-grown, 12C purified-Used to achieve long quantum coherence time
NV Center Depth~5nmDistance from surface, optimized for E-field coupling
Electron Spin Coherence Time (T2)1.6msMeasured using exponential attenuation fit
Ground State Splitting (D)2.87GHzZero-field splitting of the 3A2 state
Applied Axial Magnetic Field (Bz)181.47GUsed to lift the
Transverse Electric Dipole Moment (d⊄)17 ± 3Hz/(V·cm-1)Key coupling constant for E-field control
E-field Driven Ļ€ Pulse Duration (τπ)6.65µsAchieved at 0.28 W source power
E-field Source Power (W)0.28WMaximum power used for fastest ERabi
ERabi Frequency Scaling FitfERabi = 257.129√W - 0.176kHzEmpirical relationship derived from experimental data
Electrode Gap10µmDistance between surface gold electrodes
Air Breakdown Limit (Current)~30kV/cmLimits current E-field strength and control speed
Diamond Breakdown Limit (Potential)21.5MV/cmTheoretical maximum E-field strength if electrodes are embedded

The experiment utilized a highly purified diamond sample and specialized electrode structures integrated onto an Optically Detected Magnetic Resonance (ODMR) platform.

  1. Material Preparation:

    • Diamond was grown via Chemical Vapor Deposition (CVD) and purified to 99.999% 12C to maximize electron spin coherence time (T2).
    • NV centers were created via 2.5 keV 15N ion implantation, resulting in NV centers approximately 5 nm below the surface to enhance coupling with the surface electrodes.
  2. Electrode Fabrication:

    • A pair of gold (Au) electrodes were deposited directly onto the diamond surface.
    • The electrode gap was approximately 10 µm, designed to generate a strong, localized alternating electric field (E-field) when driven by a microwave source (MWE).
    • A separate gold stripline, placed 10 µm away from the electrodes, was used for conventional magnetic control (MWB).
  3. Spin Initialization and Readout:

    • A 532 nm laser was used for spin initialization (polarizing the spin to the |ms = 0> state) and readout (measuring fluorescence intensity, where |0> is bright and |±1> is dark).
    • The system was operated on a laser scanning confocal microscope platform integrated with ODMR technology.
  4. E-field Driven Rabi Oscillation (ERabi) Sequence:

    • Initialization: 532 nm laser pulse polarizes the spin to |0>.
    • Preparation: A resonant microwave magnetic Ļ€-pulse (MWB) drives the spin from |0> to the |-1> state.
    • Coherent Control: An alternating E-field pulse (PE) is applied for a variable duration (Ļ„), driving the coherent oscillation between |-1> and |+1> (Delta ms = ±2).
    • Readout: A final MWB Ļ€-pulse transfers the remaining population in the |-1> state back to |0> for fluorescence measurement. The resulting fluorescence contrast reveals the population transfer driven by the E-field.

The ability to coherently control NV center spins using localized electric fields is crucial for the development and commercialization of solid-state quantum technologies.

Industry/FieldApplicationTechnical Relevance
Quantum ComputingSolid-State Qubit Control, Quantum Logic GatesE-field control allows for fast, localized, and scalable qubit addressing, essential for dense integration on semiconductor platforms.
Quantum Sensing (Electromagnetism)High-Resolution Electric Field SensingThe demonstrated strong coupling between the E-field and the spin state forms the basis for highly sensitive, nanoscale E-field sensors.
Quantum SimulationIntegrated Quantum SystemsEnables the study of complex quantum phenomena in solid-state environments using highly controllable, integrated NV centers.
Micro/Nano-ElectronicsHybrid Quantum-Classical DevicesE-field control is inherently compatible with CMOS fabrication, facilitating the integration of NV quantum sensors directly onto classical electronic circuits.
Precision MeasurementTemperature and Strain SensingWhile the paper focuses on E-field, the underlying NV platform is used for high-precision measurement of temperature, strain, and magnetic fields (as demonstrated by the related articles). E-field control enhances the speed and fidelity of these sensing protocols.
View Original Abstract

The nitrogen-vacancy (NV) color center quantum system in diamond has shown great application potential in the fields of solid-state quantum computing and quantum precision measurement because of its unique advantages such as single-spin addressing and manipulation and long quantum coherence time at room temperature. The precise manipulation technology of single spin is particularly important for the development of the application of NV center. The common spin manipulation methods used in NV center quantum system are to drive and manipulate the electron spin by resonant alternating magnetic field. In recent years, the electrical control of quantum spin has attracted extensive attention. In this paper, using the alternating electric field to control the electron spin of NV center is studied. The alternating electric field generated by the electrode successfully drives the Rabi oscillation of the NV center spin between the <inline-formula><tex-math id=ā€œM4ā€>\begin{document}$\Delta m_{\rm{s}}=\pm2$\end{document}</tex-math><alternatives><graphic xmlns:xlink=ā€œhttp://www.w3.org/1999/xlinkā€ xlink:href=ā€œ11-20220410_M4.jpgā€/><graphic xmlns:xlink=ā€œhttp://www.w3.org/1999/xlinkā€ xlink:href=ā€œ11-20220410_M4.pngā€/></alternatives></inline-formula> magnetic-dipole forbidden energy levels of <inline-formula><tex-math id=ā€œM5ā€>\begin{document}$|m_{\rm{s}}=-1\rangle$\end{document}</tex-math><alternatives><graphic xmlns:xlink=ā€œhttp://www.w3.org/1999/xlinkā€ xlink:href=ā€œ11-20220410_M5.jpgā€/><graphic xmlns:xlink=ā€œhttp://www.w3.org/1999/xlinkā€ xlink:href=ā€œ11-20220410_M5.pngā€/></alternatives></inline-formula> and <inline-formula><tex-math id=ā€œM6ā€>\begin{document}$|m_{\rm{s}}=+1\rangle$\end{document}</tex-math><alternatives><graphic xmlns:xlink=ā€œhttp://www.w3.org/1999/xlinkā€ xlink:href=ā€œ11-20220410_M6.jpgā€/><graphic xmlns:xlink=ā€œhttp://www.w3.org/1999/xlinkā€ xlink:href=ā€œ11-20220410_M6.pngā€/></alternatives></inline-formula>. Further studies show that the frequency of the electrically driven Rabi oscillation is controlled by the power of the driven electric field but independent of the resonant frequency of the electric field. The combination of spin electric control and magnetic control technology can realize the full manipulation of the direct transition among the three spin energy levels of NV center, thus promoting the development of the researches and applications of NV quantum system in the fields of quantum simulation, quantum computing, precision measurement of electromagnetic field, etc.