All-microwave holonomic control of an electron-nuclear two-qubit register in diamond
At a Glance
Section titled âAt a Glanceâ| Metadata | Details |
|---|---|
| Publication Date | 2020-04-20 |
| Journal | Physical review. B./Physical review. B |
| Authors | V. O. Shkolnikov, Roman Mauch, Guido Burkard |
| Institutions | University of Konstanz |
| Citations | 11 |
| Analysis | Full AI Review Included |
Technical Documentation & Analysis: All-Microwave Holonomic Control in Diamond
Section titled âTechnical Documentation & Analysis: All-Microwave Holonomic Control in DiamondâThis document analyzes the research detailing the universal holonomic control of a two-qubit register (NV electron spin and nearby 13C nuclear spin) in diamond using only microwave pulses. This application requires ultra-high-purity Single Crystal Diamond (SCD) with precise isotopic control, a core capability of 6CCVD.
Executive Summary
Section titled âExecutive SummaryâThe research demonstrates a robust, all-microwave scheme for universal quantum gates on a diamond NV center two-qubit register.
- Qubit Register: Utilizes the electron spin of the Nitrogen-Vacancy (NV-) center coupled to the spin of a nearest-neighbor 13C nuclear atom.
- Control Mechanism: Achieves universal holonomic (geometric) gates using only microwave pulses, eliminating the need for slower radio frequency (RF) control.
- Speed and Fidelity: Simulated gate operation times are fast (~285 ns), limited by the 36 MHz resonance splitting, achieving high fidelity (up to 0.995) under realistic detuning noise.
- Key Innovation: Applying a precise axial magnetic field ($B_z = D_{gs}/\gamma_e$) mixes the electronic states $|-1\rangle$ and $|0\rangle$, allowing microwave fields to efficiently drive transitions previously forbidden by nuclear spin selection rules.
- Material Requirement: Requires high-quality Single Crystal Diamond (SCD) with controlled 13C isotopic concentration to ensure strong, addressable hyperfine coupling.
- Initialization: Coherent Population Trapping (CPT) protocol achieves 98% initialization fidelity in 100 ”s.
Technical Specifications
Section titled âTechnical SpecificationsâThe following hard data points are extracted from the analysis of the NV ground state and the proposed operating regime.
| Parameter | Value | Unit | Context |
|---|---|---|---|
| NV Ground State Zero-Field Splitting ($D_{gs}$) | 2.88 | GHz | Fundamental NV property |
| Electronic Gyromagnetic Ratio ($\gamma_e$) | 2.8 | MHz/G | Used in Hamiltonian $H_e$ |
| Nuclear Gyromagnetic Ratio ($\gamma_n$) | 0.001 | MHz/G | 13C nuclear spin |
| Closest 13C Hyperfine Axial Coupling ($A_{zz}$) | 201 | MHz | Nearest neighbor 13C atom |
| Required Axial Magnetic Field ($B_z$) | $D_{gs}/\gamma_e$ | G | Approx. 1028 G; sets $ |
| Transverse Magnetic Field ($B_\perp$) | 500 | G | Used in initialization simulation |
| Closest Resonance Frequency Difference | 36 | MHz | Sets the limit for gate speed |
| Gate Operation Time ($\tau$) | ~285 | ns | Time required for CNOT gate |
| Initialization Fidelity | 98 | % | Achieved in 100 ”s using CPT protocol |
| Simulated Average Gate Fidelity (Detuning Error) | 0.995 | N/A | CNOT gate on electron spin |
| Simulated Average Gate Fidelity (Energy Fluctuation Error) | 0.985 | N/A | CNOT gate on electron spin |
Key Methodologies
Section titled âKey MethodologiesâThe experiment relies on precise material engineering and complex electromagnetic control protocols.
- Material Selection: Use of high-purity diamond hosting NV centers, specifically requiring the presence of 13C nuclear spins (either natural abundance or isotopically enriched) to form the two-qubit register via strong hyperfine interaction.
- Magnetic Field Tuning: Application of a strong axial magnetic field ($B_z$) tuned precisely to the zero-field splitting ratio ($D_{gs}/\gamma_e$) to achieve degeneracy between the $|-1\rangle$ and $|0\rangle$ electronic states.
- State Mixing: Application of a nonparallel magnetic field ($B_\perp$) to mix the electronic states, creating new eigenstates $|+\rangle$ and $|-\rangle$ separated by $|\Omega|$.
- Microwave Control: Implementation of eight distinct microwave pulse protocols ($P_1$ through $P_8$) tuned to the specific hyperfine resonance frequencies (separated by $\ge 36$ MHz) to achieve universal holonomic control.
- Initialization Protocol: Coherent Population Trapping (CPT) using simultaneous optical fields (resonant with the 1.945 eV Zero Phonon Line) and microwave tones to rapidly pump the system into the lowest hyperfine ground state with 98% fidelity.
6CCVD Solutions & Capabilities
Section titled â6CCVD Solutions & Capabilitiesâ6CCVD is uniquely positioned to supply the foundational diamond materials and custom engineering required to replicate and advance this high-fidelity quantum control research.
Applicable Materials
Section titled âApplicable MaterialsâThe success of this research hinges on the quality and isotopic purity of the diamond substrate. 6CCVD recommends the following:
- Optical Grade Single Crystal Diamond (SCD): Required for high-fidelity optical initialization and readout (1.945 eV ZPL). Our SCD features extremely low nitrogen content (< 1 ppb) to minimize background noise and maximize NV coherence time ($T_2$).
- Controlled Isotopic Purity: The two-qubit register relies on the 13C nuclear spin. 6CCVD offers:
- Natural Abundance 13C SCD: For projects utilizing randomly distributed nearest-neighbor 13C atoms.
- Isotopically Enriched 12C SCD: For applications requiring long $T_2$ coherence times, where 13C is intentionally minimized.
- Custom 13C Doping: For targeted research requiring specific, higher concentrations of 13C to increase the probability of finding strongly coupled nuclear spins.
Customization Potential
Section titled âCustomization PotentialâThe implementation of all-microwave control often requires integrated on-chip structures for efficient microwave delivery.
| Research Requirement | 6CCVD Custom Capability | Benefit to Researcher |
|---|---|---|
| High-Quality Optical Access | Polishing: SCD surfaces polished to Ra < 1 nm. | Maximizes photon collection efficiency and minimizes scattering losses during optical initialization. |
| Microwave Pulse Delivery | Custom Metalization: Internal capability for deposition of Au, Pt, Ti, Cu, etc. | Allows researchers to fabricate on-chip microwave structures (e.g., coplanar waveguides) directly onto the diamond surface for precise field control. |
| Large-Scale Integration | Custom Dimensions: Plates/wafers up to 125 mm (PCD) and large SCD substrates (up to 10 mm thickness). | Supports scaling up the quantum register or integrating multiple NV devices on a single platform. |
| Device Fabrication | Laser Cutting/Shaping: Precision cutting services for unique geometries or mesa structures. | Enables integration into complex cryogenic or magnetic field setups. |
Engineering Support
Section titled âEngineering SupportâThe theoretical scheme relies on complex perturbation theory and precise magnetic field tuning to achieve the required state mixing and resonance conditions ($B_z = D_{gs}/\gamma_e$).
6CCVDâs in-house PhD team specializes in the material science of NV centers and diamond growth parameters. We offer consultation on:
- Material Selection: Optimizing nitrogen and 13C concentration to balance high coherence ($T_2$) with strong, addressable hyperfine coupling ($A_{ij}$).
- Surface Termination: Ensuring optimal surface quality to maintain the NV- charge state stability critical for long-term qubit operation.
- Substrate Preparation: Providing substrates with specific crystallographic orientations necessary for alignment with external magnetic fields.
For custom specifications or material consultation, visit 6ccvd.com or contact our engineering team directly.
View Original Abstract
We present a theoretical scheme that allows to perform a universal set of\nholonomic gates on a two qubit register, formed by a $^{13}$C nuclear spin\ncoupled to the electron spin of a nitrogen-vacancy center in diamond. Strong\nhyperfine interaction between the electron spin and the spins of the first\nthree shells of $^{13}$C atoms allows to operate the state of the register on\nthe submicrosecond timescale using microwave pulses only. We describe the\nsystem and the operating regime analytically and numerically, as well as\nsimulate the initialization protocols.\n