Demonstration of the Holonomically Controlled Non-Abelian Geometric Phase in a Three-Qubit System of a Nitrogen Vacancy Center
At a Glance
Section titled âAt a Glanceâ| Metadata | Details |
|---|---|
| Publication Date | 2022-11-02 |
| Journal | Entropy |
| Authors | Shaman Bhattacharyya, Somnath Bhattacharyya |
| Institutions | University of the Witwatersrand |
| Citations | 3 |
| Analysis | Full AI Review Included |
Executive Summary
Section titled âExecutive SummaryâThis study demonstrates the successful simulation and analysis of holonomically controlled non-Abelian geometric phase gates on a three-qubit Nitrogen Vacancy (NV) center system, validating a robust approach for universal quantum computation.
- Core Achievement: Simulation of universal holonomic control on a three-qubit, eight-level NV center system using the IBM Quantum Experience (IBM QE) platform.
- Fidelity Improvement: Off-resonant holonomic gates achieved a high fidelity of approximately 85%, significantly outperforming on-resonant gates, which reached only ~70% fidelity.
- Decoherence Control: The transition between the systemâs three dark states was demonstrated, showing that decoherence is minimized when the gateâs dark state aligns with the qubitâs initial state, achieved via a specific Ï/3 rotation.
- Non-Abelian Phase Generation: The concatenation of three separate Abelian rotation paths effectively produced a non-Abelian geometric phase, which is inherently resilient to local noise and errors.
- Viability Confirmation: The results support the use of NV centers in diamond as highly viable, room-temperature solid-state qubits for developing universal, fault-tolerant quantum computers.
Technical Specifications
Section titled âTechnical Specificationsâ| Parameter | Value | Unit | Context |
|---|---|---|---|
| Qubit System Type | Nitrogen Vacancy (NV) Center | N/A | Solid-state spin qubits in diamond |
| System Size (Simulated) | 3 | Qubits | Modeled as an eight-level system |
| Simulation Platform | IBM Q 14 Melbourne | Device | Actual quantum hardware used for digital simulation |
| Gate Type | Holonomic (Non-Abelian) | N/A | Gates based on geometric phase accumulation |
| Off-Resonant Gate Fidelity | ~85 | % | Maximum achieved fidelity for 3-qubit HQC |
| On-Resonant Gate Fidelity | ~70 | % | Comparative fidelity, demonstrating superiority of off-resonance |
| Qubit 1 Rabi Frequency (Ω) | 4966 | MHz | Frequency used for holonomic gate implementation |
| Decoherence Control Rotation | Ï/3 (60) | Radians (Degrees) | Rotation angle used to align the gateâs dark state |
| Optimal Dark State Alignment Detuning (Î) | 450 | MHz | Detuning frequency (Î1) where dark state alignment minimizes deviation |
| Phase Dependence | Detuning Frequency (Î) | N/A | Geometric phase magnitude varies as a function of Î |
Key Methodologies
Section titled âKey MethodologiesâThe holonomic control of the three-qubit NV center system was demonstrated through a sequence of quantum simulations and calculations on the IBM QE platform:
- System Initialization and Modeling: The three-qubit system was modeled using the Greenberger-Horne-Zeilinger (GHZ) frame of reference. Qubits were initialized using identity gates, followed by Rx and Rz gates to set the rotation parameters (Ξ and Ï).
- Holonomic Gate Implementation: The unitary holonomic gate (U) was implemented using standard quantum gates (Rx, Ry, Rz) combined with simulated detuning pulses (Î) and Rabi frequencies (Ω) applied to all three qubits.
- Rotation Path Concatenation: Three separate rotation pathsâone for each qubitâwere defined and concatenated. The first two qubits underwent complete rotations (Ξ = ±2Ï), while the third qubit rotated around a circular path (Ξ ranging between Ï/6 and -Ï/6).
- Off-Resonance Optimization: The detuning frequencies (Î1, Î2, Î3) were varied to move the gate operation off-resonance. This variation was critical for maximizing the accumulated geometric phase and improving gate fidelity.
- Dark State Analysis: The alignment of the gateâs dark state with the initial qubit state was analyzed by observing the return probability (Pr) as a function of detuning frequency and time. The minimum deviation point (450 MHz) confirmed optimal decoherence control.
- Fidelity Calculation: Gate performance was quantified using the fidelity formula F(Ï,Îș) = Tr[ââÏ Îș âÏ], comparing the ideal density matrix (Ï) from the QasmSimulator with the experimental density matrix (Îș) obtained from the IBM Q 14 Melbourne device.
Commercial Applications
Section titled âCommercial ApplicationsâThe development of robust, high-fidelity holonomic gates on solid-state NV centers has direct implications for several advanced technological sectors:
- Universal Quantum Computing: Provides a pathway for building fault-tolerant quantum processors, particularly solid-state devices based on diamond, which can operate at room temperature.
- Quantum Sensing and Metrology: NV centers are premier quantum sensors. Holonomic control enhances the robustness of these sensors against environmental noise, leading to higher precision magnetometers, thermometers, and gyroscopes.
- Fault-Tolerant Quantum Memory: Geometric phases are inherently robust against noise, making holonomic gates ideal for implementing quantum memory and error correction codes (e.g., holonomic surface codes).
- Spin-Orbitronics and Topological Materials: The simulation of non-Abelian geometric phases and dark states relates directly to understanding Rashba spin-orbit coupling (RSOC) and vortex structures in topologically protected materials.
- Microwave and RF Control Systems: The technique relies on precise control using microwave and radiofrequency pulses, applicable to advanced signal processing and quantum communication hardware.
View Original Abstract
The holonomic approach to controlling (nitrogen-vacancy) NV-center qubits provides an elegant way of theoretically devising universal quantum gates that operate on qubits via calculable microwave pulses. There is, however, a lack of simulated results from the theory of holonomic control of quantum registers with more than two qubits describing the transition between the dark states. Considering this, we have been experimenting with the IBM Quantum Experience technology to determine the capabilities of simulating holonomic control of NV-centers for three qubits describing an eight-level system that produces a non-Abelian geometric phase. The tunability of the geometric phase via the detuning frequency is demonstrated through the high fidelity (~85%) of three-qubit off-resonant holonomic gates over the on-resonant ones. The transition between the dark states shows the alignment of the gateâs dark state with the qubitâs initial state hence decoherence of the multi-qubit system is well-controlled through a Ï/3 rotation.
Tech Support
Section titled âTech SupportâOriginal Source
Section titled âOriginal SourceâReferences
Section titled âReferencesâ- 1999 - Holonomic quantum computation [Crossref]
- 2014 - Non-Abelian geometric phase in the diamond nitrogen-vacancy center [Crossref]
- 2018 - Holonomic surface codes for fault-tollerant quantum computation [Crossref]
- 2009 - Operator fidelity susceptibility: An indicator of quantum criticalitym [Crossref]
- 2014 - Room temperature high-fidelity holonomic single-qubit gate on a solid-state spin [Crossref]
- 2015 - Universal holonomic quantum gates in decoherence-free subspace on superconducting circuits [Crossref]
- 2019 - Nonadiabatic holonomic multiqubit controlled gates [Crossref]
- 2018 - Direct evidence for hula twist and single-bond rotation photoproducts [Crossref]
- 2017 - Holonomic quantum control by coherent optical excitation in diamond [Crossref]