Quantum information processing with nuclear spins mediated by a weak-mechanically controlled electron spin
At a Glance
Section titled âAt a Glanceâ| Metadata | Details |
|---|---|
| Publication Date | 2022-02-21 |
| Journal | Communications in Theoretical Physics |
| Authors | Wan-Jun Su, Guang-Zheng Ye, Yadong Wu, ZhenâBiao Yang, Barry C. Sanders |
| Institutions | University of Calgary, University of Hong Kong |
| Analysis | Full AI Review Included |
Executive Summary
Section titled âExecutive SummaryâThis research proposes a robust scheme for achieving quantum information processing (QIP) using nuclear spins in diamond, mediated by a mechanically controlled Nitrogen-Vacancy (NV) center electron spin.
- Core Value Proposition: Achieves high-fidelity two-qubit entangling gates and Quantum State Transfer (QST) between distant nuclear spins (e.g., 13C) using a weak mechanical drive, overcoming challenges related to small coupling coefficients and positional disorder.
- Mediation Mechanism: The NV center electron spin acts as a mediator, coupling two nuclear spins via magnetic dipole-dipole interactions.
- Control Method: A gigahertz-frequency mechanical (stress) wave is used to drive the magnetically forbidden spin transition (|ms = -1> â |ms = +1>) of the NV center.
- Robustness via Zeno Dynamics: The scheme operates in the Quantum Zeno regime, where the driving Rabi frequency (Ω) is much smaller than the dipole-coupling strength (g). This confines the system evolution to a quantum dark subspace (Z0), making the gates robust against decoherence and positional uncertainties (fluctuating distances, r).
- Performance Metrics: The required gate operation time is fast (T â 2.5 ”s), which is significantly shorter than the typical T1 and T2 coherence times of the nuclear spins, leading to high fidelity (F > 0.96).
Technical Specifications
Section titled âTechnical Specificationsâ| Parameter | Value | Unit | Context |
|---|---|---|---|
| NV Center Zero-Field Splitting (D) | 2.87 | GHz | Energy gap between |
| Dipole-Coupling Strength (g) | ~2Ï x 2 | MHz | Interaction between 14NV electron spin and 13C nuclear spin. |
| Driving Rabi Frequency (Ω) | ~2Ï x 210 | kHz | Mechanical (stress) wave driving the |
| Optimized Driving Ratio (Ω/g) | 0.1 | N/A | Ratio chosen to balance high fidelity and short operating time. |
| Gate Operation Time (T) | ~2.5 | ”s | Required time for entangling gate or QST (T = Ï/Ω). |
| NV Spontaneous Decay Rate (ÎNV) | ~1 | KHz | Used in numerical simulations. |
| Nuclear Spin Dephasing Rate (ÎłN) | ~1/3 | KHz | Used in numerical simulations. |
| Required NV T2 (Room Temp) | > 600 | ”s | Coherence time required for high-fidelity operation. |
| QST Fidelity (Robustness) | â„ 0.98 | N/A | Achieved despite 10% fluctuations in coupling strength (ÎŽg/g) and time (ÎŽt/t). |
| Average Gate Fidelity (Detuning) | 0.995 | N/A | Achieved with scaled off-resonant coupling Î/Ω = 0.1. |
Key Methodologies
Section titled âKey MethodologiesâThe protocol relies on precise initialization and control of the NV center spin using mechanical waves while leveraging the strong dipole coupling to enforce Zeno dynamics.
- System Setup: An NV center electron spin is positioned to mediate magnetic dipole-dipole interaction between two nearby nuclear spins (e.g., 13C) in a diamond lattice.
- NV Spin Initialization: The NV center is initialized into the |ms = 0> state via linearly polarized optical excitation. This state is then robustly transferred to the required initial state, |ms = +1> (|f>NV), using a magnetic adiabatic passage technique.
- Mechanical Driving Application: A gigahertz-frequency mechanical (stress) wave is applied, tuned to the resonance frequency (ÏHBAR), to drive the magnetically forbidden spin transition |ms = +1> â |ms = -1> of the NV center.
- Quantum Zeno Regime Enforcement: The driving field Rabi frequency (Ω) is intentionally kept weak relative to the dipole-coupling strength (g), satisfying the condition Ω << g. This ensures a large energy splitting (ÎE >> Ω) that confines the system evolution to the zero-energy dark subspace (Z0).
- Gate Execution: The entangling gate or QST is executed by maintaining the weak mechanical drive for a precise duration T = Ï/Ω. The system coherently evolves within the dark subspace, achieving the desired nuclear-nuclear interaction indirectly.
Commercial Applications
Section titled âCommercial Applicationsâ| Industry/Application | Relevance to Technology |
|---|---|
| Solid-State Quantum Computing | Nuclear spins offer superior coherence times compared to electron spins, making them ideal for long-term quantum memory (qubit storage) in diamond-based quantum processors. |
| Scalable Quantum Architecture | Provides a robust method for generating multi-nuclear-spin gates and multi-party communication, essential for scaling up quantum systems beyond two qubits. |
| Quantum State Transfer (QST) | Enables reliable, high-fidelity transfer of quantum information between distant nuclear qubits, a fundamental requirement for building distributed quantum networks. |
| Nanoscale Quantum Sensing | The NV center acts as a sensitive dipole âantenna,â allowing detection and characterization of nuclear spins at different spatial locations, applicable in detecting charge recombination rates in radical pair reactions. |
| Chemical and Biological Probes | The robust coupling mechanism can be used to study structural information of nuclear spins in single molecules, offering high-resolution sensing for chemical and biological processes. |
| Advanced Diamond Materials | Requires high-purity diamond substrates (e.g., those produced by specialized CVD techniques) with precise control over NV center placement and the concentration of 13C nuclear spins. |
View Original Abstract
Abstract We propose a scheme to achieve nuclear-nuclear indirect interactions mediated by a mechanically driven nitrogen-vacancy (NV) center in a diamond. Here we demonstrate two-qubit entangling gates and quantum-state transfer between two carbon nuclei. When the dipole-dipole interaction strength is much larger than the driving field strength, the scheme is robust against decoherence caused by coupling between the NV center (nuclear spins) and the environment. Conveniently, precise control of dipole coupling is not required so this scheme is insensitive to fluctuating positions of the nuclear spins and the NV center. Our scheme provides a general blueprint for multi-nuclear-spin gates and for multi-party communication.