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Spin-defect qubits in two-dimensional transition metal dichalcogenides operating at telecom wavelengths

MetadataDetails
Publication Date2022-12-06
JournalNature Communications
AuthorsYeonghun Lee, Yaoqiao Hu, Xiuyao Lang, Dongwook Kim, Kejun Li
InstitutionsThe University of Texas at Dallas, University of Washington
Citations39
AnalysisFull AI Review Included

This research computationally discovers and characterizes a promising family of spin-defect qubits (MX family) realized in two-dimensional (2D) Transition Metal Dichalcogenides (TMDs), specifically optimized for quantum network applications.

  • Telecom Operation: The defects, such as WSe in MoSe2, exhibit Zero-Phonon Line (ZPL) optical transitions in the highly desirable telecom band (0.74-0.94 eV or 1260-1675 nm), enabling long-distance quantum communication via standard optical fibers.
  • High Zero-Field Splitting (ZFS): The defects possess a large spin-triplet ground state with ZFS values typically ranging from 10 to 20 GHz, significantly higher than the NV center in diamond, facilitating robust microwave control and high-temperature resonant spin readout.
  • Fast Radiative Decay: Calculated radiative lifetimes (TR) are in the microsecond range (e.g., 4.2 ”s for WSe in MoSe2), which is 100 to 1000 times faster than the NV center in diamond, supporting efficient spin initialization and readout.
  • 2D Integration Advantage: The 2D host material allows for seamless monolithic integration with semiconductor electronics, heterostructure engineering, and precise defect placement (e.g., via STM lithography).
  • Strain Tunability: The ZPL energy and radiative lifetime can be finely tuned by applying mechanical strain (uniaxial or biaxial), offering a method to minimize transmission loss and create highly sensitive quantum strain sensors.
  • Low Nuclear Spin Noise: TMD hosts offer reduced sensitivity to nuclear spin environments and the feasibility of isotopic purification, promising long spin coherence times (T2).

The following data was derived from hybrid Density Functional Theory (DFT) calculations, primarily focusing on the WSe defect in monolayer MoSe2.

ParameterValueUnitContext
Defect FamilyMXN/ATransition metal substituted at chalcogen site
Primary Host MaterialMoSe2N/AMonolayer Transition Metal Dichalcogenide
Primary DefectWSeN/ATungsten substituted at Selenium site
Zero-Phonon Line (ZPL) Energy0.74eVWSe in MoSe2 (SOC corrected)
ZPL Wavelength (WSe in MoSe2)~1675nmFalls within the telecom band
ZPL Energy (WS in MoS2)0.94eVWS in MoS2 (SOC corrected)
Zero-Field Splitting (D) Range10-20GHzGeneral range for MX defect family
ZFS (WSe in MoSe2)7.23GHzCalculated D value
Radiative Lifetime (TR)4.2”sWSe in MoSe2
Radiative Lifetime (TR)20.5”sWS in MoS2
Intersystem Crossing (ISC) Time0.031”sTISC (WSe in MoSe2), faster than TR
Strain Tuning Capability (ΔE)HundredsmeVModulation of energy gap (a1 to ex,y) under strain
Host Point Group SymmetryC3vN/ASymmetry of the defect environment
Telecom Band Range1260-1675nmLow-loss optical fiber transmission window

The discovery and characterization of the MX defect family were achieved through systematic first-principles computational methods, primarily based on Density Functional Theory (DFT).

  1. Initial Screening: DFT calculations using the Perdew-Burke-Ernzerhof (PBE) functional were performed to identify defects meeting two criteria: (i) spin-triplet ground state, and (ii) spin-conserving intradefect optical transition without ionization.
  2. Hybrid DFT Calculations: Detailed electronic structures were computed using the Vienna Ab initio Simulation Package (VASP) employing the Heyd-Scuseria-Ernzerhof (HSE06) hybrid functional to accurately model bandgaps and defect energy levels.
  3. Supercell Setup: Monolayer TMDs (MoS2, MoSe2, etc.) were modeled using 6 x 6 x 1 primitive supercells, including a 15-Angstrom vacuum region to simulate the 2D environment.
  4. Defect Formation Energy: Defect formation energies were calculated using the COFFEE (Corrections For Formation Energy and Eigenvalues) code, which applies the FNV (Freysoldt-Neugebauer-Van de Walle) charge correction scheme to account for electrostatic interactions in charged supercells.
  5. Magnetic Properties Calculation: VASP subroutines were utilized to compute the magnetic properties, including the Zero-Field Splitting (ZFS) tensors and the hyperfine tensors (A(n)).
  6. Optical and Vibrational Properties: Configuration coordinate diagrams were generated using constrained-occupation DFT to model the Zero-Phonon Line (ZPL) emission and estimate the Huang-Rhys factor (S).
  7. Intersystem Crossing (ISC) Rate: The ISC rate was calculated using Fermi’s golden rule, requiring the computation of Spin-Orbit Coupling (SOC) strength via the ORCA code (using time-dependent DFT and cluster models) and phonon wavefunction overlap.
  8. Strain Engineering Simulation: Uniaxial and biaxial strains (up to ±3%) were applied computationally to the host materials to determine the resulting modulation of radiative lifetime (TR) and ZPL energy (ΎE).

The unique combination of telecom operation, high ZFS, and 2D integration capability positions the MX defect family for several advanced engineering and quantum technology applications.

  • Quantum Communication and Networks:

    • Long-Distance QKD: Direct operation in the 1260-1675 nm telecom band allows for seamless integration with existing low-loss optical fiber infrastructure, enabling the realization of long-distance quantum entanglement networks.
    • Quantum Repeaters: The defects serve as promising solid-state quantum memory nodes for storing and transmitting quantum information.
  • Integrated Quantum Devices:

    • Monolithic Hybrid Devices: The 2D nature of the host materials facilitates integration with conventional 3D semiconductor electronic devices, enabling the creation of scalable, monolithically integrated hybrid classical-quantum systems.
    • Photonic Integration: Ease of integration with on-chip photonic platforms (waveguides, cavities) allows for enhanced photon collection efficiency via the Purcell effect, compensating for moderate oscillator strengths.
  • Quantum Sensing and Metrology:

    • Quantum Strain Sensors: The drastic and sensitive shift of defect energy levels under small uniaxial strain makes these defects highly susceptible quantum strain sensors.
    • High-Temperature Sensing: The large ZFS (10-20 GHz) enables resonant spin readout and control at higher temperatures compared to defects with smaller ZFS.
  • Advanced Manufacturing and Lithography:

    • Precision Defect Placement: The ability to place defects precisely within a 2D layer (versus being buried in 3D bulk) using techniques like Scanning Tunneling Microscope (STM) or focused electron beam lithography is critical for manufacturing scalable quantum registers.