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Symmetric carbon tetramers forming spin qubits in hexagonal boron nitride

MetadataDetails
Publication Date2023-10-11
Journalnpj Computational Materials
AuthorsZsolt Benedek, Rohit Babar, Ádám Ganyecz, Tibor Szilvási, Örs Legeza
InstitutionsHUN-REN Wigner Research Centre for Physics, University of Alabama
Citations23
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Technical Documentation & Analysis: Spin Qubits in hBN

Section titled “Technical Documentation & Analysis: Spin Qubits in hBN”

This research proposes the symmetric carbon tetramer defects (C4N and C4B) in hexagonal boron nitride (hBN) as novel spin qubits for atomic-scale, low-dimensional quantum sensing, offering a potential alternative or complement to established 3D systems like the Nitrogen-Vacancy (NV) center in diamond.

  • Core Achievement: Theoretical prediction of high-spin triplet ground states in neutral C4N and C4B defects in hBN, suitable for Optical Detection of Magnetic Resonance (ODMR).
  • Enhanced Sensitivity: The defects exhibit a remarkably narrow Electron Spin Resonance (ESR) linewidth (as low as 8 MHz for C4N in 11BN), which is critical for achieving high quantum sensing sensitivity.
  • Optical Readout: The C4N defect shows a Zero Phonon Photoluminescence Line (ZPL) at 2.18 eV (~590 nm), enabling optical spin state initialization and readout in the visible spectrum.
  • Strain Engineering: The C4N defect’s spin-selective decay is highly sensitive to out-of-plane distortions (buckling), demonstrating that mechanical strain can be used to engineer intersystem crossing rates and tailor spin contrast.
  • Material Stability: The C4N and C4B defects show high energy barriers against complex formation with carbon interstitials, suggesting thermal stability up to ~630 K.
  • 6CCVD Value Proposition: While this study focuses on hBN, 6CCVD provides the industry-leading MPCVD Single Crystal Diamond (SCD) platform, the established benchmark for NV and SiV quantum sensing, offering superior purity, thermal management, and integration capabilities for next-generation quantum devices.

The following hard data points were extracted from the theoretical modeling of the C4N and C4B defects in hBN:

ParameterValueUnitContext
C4N ZFS Parameter (D)820MHzZero-Field Splitting (CASSCF-NEVPT2)
C4B ZFS Parameter (D)660MHzZero-Field Splitting (CASSCF-NEVPT2)
C4N ESR Linewidth (11B)8 / 12MHzFull Width at Half Maximum (FWHM) in 11BN sample
C4B ESR Linewidth (11B)24 / 31MHzFWHM in 11BN sample
C4N ZPL Energy (Theoretical)2.18eVZero Phonon Photoluminescence Line
C4N Emission Wavelength~590nmVisible Range Optical Readout
C4N Radiative Lifetime (0 K)80.5nsTriplet Excited State
C C-Bond Stretching Modes0.196eVHighly localized vibrational modes (1583 cm-1)
C4N Formation Energy (N-rich)2.5eVNeutral Charge State
C4B Formation Energy (B-rich)2.9eVNeutral Charge State
Spin-Orbit Coupling (C4B)48.81 / 27.08GHzBetween 3A” (ms = ±1) and 1E’ / 1A’1 states

The theoretical analysis relied on a combination of periodic Density Functional Theory (DFT) and high-level quantum chemistry approaches to ensure reliability across electronic, optical, and spin properties.

  1. Periodic DFT (VASP Package): Employed for supercell modeling (162-atom monolayer and 768-atom bulk models).
    • Functional: HSE06 hybrid exchange-correlation functional (0.32 exact exchange fraction).
    • Basis Set: Plane wave basis set of 450 eV.
    • Corrections: D3 correction by Grimme et al. for van der Waals interaction.
    • ZPL Calculation: Calculated using spin-conserved constrained DFT.
  2. Quantum Chemistry (ORCA 5.0.3): Used for molecule models (small and large flakes) to calculate electronic energies, properties, and phononic effects.
    • Geometry Optimization: Performed using DFT at PBEO/cc-pVDZ level with D3(BJ) dispersion correction.
    • Excited States: Time-dependent DFT (TD-DFT) requested with ten roots; singlet excited states generated via spin-flip method.
  3. High-Level Correlation (CASSCF-NEVPT2): Used for single-point energies, dynamic correlation, and spin properties.
    • Active Space: Constructed based on TD-DFT and Density Matrix Renormalization Group (DMRG) results.
    • Spin Properties: Spin-orbit coupling (SOC) matrix elements, spin-spin coupling (SSC), and Zero-Field Splitting (ZFS) tensors calculated using Quasi-Degenerate Perturbation Theory (QDPT).
  4. ESR Spectrum Simulation: Implemented a fast Monte Carlo method, generating 2-10 million random spin state configurations to calculate the ESR line shape and hyperfine structure.

This research highlights the critical need for high-purity, structurally stable host materials and precise defect engineering to realize next-generation quantum sensors. While the paper focuses on hBN, the established, high-performance platform for quantum sensing remains MPCVD Diamond, specifically the NV center, which the authors reference as the current state-of-the-art 3D sensor.

6CCVD provides the foundational diamond materials necessary to replicate, extend, and integrate this type of quantum sensing research, offering superior thermal management, chemical stability, and integration potential compared to 2D materials alone.

To advance quantum sensing projects requiring ultra-low noise environments, high coherence, and integration capability, 6CCVD recommends the following materials:

6CCVD MaterialSpecificationApplication Relevance
Optical Grade SCDHigh-purity, low nitrogen content (PPM level). Thickness: 0.1”m - 500”m.Ideal substrate for developing high-coherence NV or SiV centers (the benchmark 3D qubits). Essential for high-fidelity optical readout in the visible range.
High-Purity PCDPlates/wafers up to 125mm. Ra < 5nm polishing.Large-area integration platform for hybrid quantum systems (e.g., integrating hBN flakes onto diamond for enhanced thermal/mechanical stability).
Boron-Doped Diamond (BDD)Custom doping levels (conductive). Thickness up to 500”m.Used as conductive electrodes for advanced ODMR/ESR setups, providing integrated microwave delivery necessary for controlling spin qubits like C4N/C4B or NV centers.

The ability to engineer the local environment, as demonstrated by the strain-sensitive intersystem crossing in C4N, requires highly customized substrates and precise fabrication. 6CCVD offers full customization to meet the stringent requirements of quantum device engineering:

  • Custom Dimensions: We supply SCD and PCD plates/wafers in custom sizes, with PCD available up to 125mm diameter, facilitating large-scale device fabrication and integration.
  • Ultra-Low Surface Roughness: Achieving the necessary proximity for low-dimensional sensing requires exceptional surface quality. 6CCVD guarantees Ra < 1nm for SCD and Ra < 5nm for inch-size PCD, crucial for stable integration of 2D materials like hBN.
  • Integrated Metalization: The implementation of ODMR/ESR requires precise microwave and electrical contacts. 6CCVD offers in-house metalization services, including Au, Pt, Pd, Ti, W, and Cu deposition, allowing researchers to design and implement custom microwave strip lines directly onto the diamond substrate.
  • Strain Engineering Substrates: We can provide substrates with controlled crystallographic orientation and thickness (up to 10mm) to assist researchers in applying and studying the effects of mechanical strain on defect properties, mirroring the strain-dependent effects observed in the C4N defect.

6CCVD’s in-house team of PhD material scientists specializes in MPCVD growth and defect engineering. We offer authoritative support for projects focused on Quantum Sensing and Optically Detected Magnetic Resonance (ODMR). We assist researchers in selecting the optimal diamond grade, doping concentration, and surface preparation required to maximize qubit coherence and integration efficiency, whether for established NV centers or for hybrid systems incorporating novel 2D materials like hBN.

For custom specifications or material consultation, visit 6ccvd.com or contact our engineering team directly.

View Original Abstract

Abstract Point defect quantum bits in semiconductors have the potential to revolutionize sensing at atomic scales. Currently, vacancy-related defects are at the forefront of high spatial resolution and low-dimensional sensing. On the other hand, it is expected that impurity-related defect structures may give rise to new features that could further advance quantum sensing in low dimensions. Here, we study the symmetric carbon tetramer clusters in hexagonal boron nitride and propose them as spin qubits for sensing. We utilize periodic-DFT and quantum chemistry approaches to reliably and accurately predict the electronic, optical, and spin properties of the studied defect. We show that the nitrogen-centered symmetric carbon tetramer gives rise to spin state-dependent optical signals with strain-sensitive intersystem crossing rates. Furthermore, the weak hyperfine coupling of the defect to their spin environments results in a reduced electron spin resonance linewidth that can enhance sensitivity.