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Fully robust qubit in atomic and molecular three-level systems

MetadataDetails
Publication Date2016-12-12
JournalNew Journal of Physics
AuthorsN. Aharon, I. Cohen, Fedor Jelezko, Alex Retzker
InstitutionsUniversitÀt Ulm, Center for Integrated Quantum Science and Technology
Citations22
AnalysisFull AI Review Included

6CCVD Technical Analysis: Robust Qubit Coherence Enhancement in NV-Diamond

Section titled “6CCVD Technical Analysis: Robust Qubit Coherence Enhancement in NV-Diamond”

Based on: “Fully robust qubit in atomic and molecular three-level systems” (N Aharon et al 2016 New J. Phys. 18 123012)


This paper presents a groundbreaking method for constructing a fully robust qubit within a three-level system, specifically demonstrating its application using the Nitrogen-Vacancy (NV) center in diamond.

  • Coherence Breakthrough: The scheme achieves robustness to both external magnetic noise and controller power fluctuations, resulting in a simulated coherence time ($T_{2}$) of $\sim 1820$ ”s.
  • Performance Gain: This represents an improvement of more than two orders of magnitude ($\gt 200 \times$) over the baseline pure dephasing time ($T_{2}^{*} = 5$ ”s), pushing the qubit performance toward its fundamental lifetime limit.
  • Material System: The methodology leverages the electronic ground state spin sub-levels of the NV-center, requiring high-quality Single Crystal Diamond (SCD) substrates.
  • Novel Technique: Robustness is achieved via continuous off-resonant driving fields applied in a $\Lambda$ (three-level) configuration, simplifying implementation compared to traditional four-level continuous dynamical decoupling schemes.
  • High-Value Application: The robust qubit enables enhanced quantum sensing, particularly for high-frequency AC magnetic signals, offering significantly improved sensitivity scaling ($ \sim \sqrt{T_{2}} $).

The following parameters were utilized and achieved in the simulation of the NV-center implementation in diamond:

ParameterValueUnitContext
Material SystemNV-Center in DiamondN/AElectronic spin 1 ground state sub-levels
Zero-Field Splitting ($D$)2.87GHzIntrinsic characteristic of the NV-center
Static Magnetic Field ($g\mu_B B$)$\sim 20$GHzApplied for large Zeeman splitting ($
Rabi Frequency ($\Omega$)70MHzAmplitude of continuous driving fields
Primary Detuning ($\Delta_{1}$)500MHzOptimized off-resonance parameter
Secondary Detuning ($\Delta_{2}$)209MHzOptimized for robustness ($\Delta E_{0} = \Delta E_{B}$)
Energy Gap ($E_{BD}$)$\sim 17.96$MHzEnergy separation of dressed states
Initial Dephasing Time ($T_{2}^{*}$)5”sBaseline coherence limited by ambient noise
Achieved Coherence Time ($T_{2}$)$\sim 1820$”sSimulated result for fully robust qubit
Noise Reduction MechanismContinuous Dynamical DecouplingN/ARobustness to external magnetic and controller noise
Target ApplicationQuantum SensingN/AEnhanced sensitivity to high-frequency signals

The robust qubit construction relies on a specific configuration and precise tuning of continuous driving fields applied to the NV-center’s electronic ground state.

  1. Material Basis Selection: Utilization of the NV-center electronic spin ground state, $| m_{s} = 0 \rangle$ and $| m_{s} = \pm 1 \rangle$, which form a natural three-level system (a qutrit).
  2. Zeeman Splitting Application: A strong static magnetic field ($g\mu_B B \approx 20$ GHz) is applied along the NV axis to create a large Zeeman splitting between the $| \pm 1 \rangle$ states, resolving the $| \pm 1 \rangle \leftrightarrow | 0 \rangle$ transitions into two distinct frequencies ($\sim 23$ GHz and $\sim 17$ GHz).
  3. $\Lambda$ System Configuration: The three levels are coupled using continuous, off-resonant microwave driving fields, creating an effective robust qubit subspace (dressed states).
  4. Off-Resonant Driving Fields: The scheme utilizes red-detuned ($\Delta_{1}$) and blue-detuned ($\Delta_{2}$) microwave fields.
    • $H_{red}$ (Red Detuned): Couples $| 0 \rangle$ to $| -1 \rangle$ and $| +1 \rangle$ with detuning $\Delta_{1}$.
    • $H_{blue}$ (Blue Detuned): Couples $| 0 \rangle$ to $| -1 \rangle$ and $| +1 \rangle$ with detuning $\Delta_{2}$.
  5. Robustness Tuning: The ratio of the detunings ($\Delta_{1}$ and $\Delta_{2}$) and the Rabi frequency ($\Omega$) are precisely tuned to ensure the second-order Stark shifts of the two critical qubit states ($| 0 \rangle$ and $| B \rangle$) are identical. This eliminates first-order coupling to controller noise (driving amplitude fluctuations).
  6. High Energy Gap Maintenance: A large energy gap ($E_{BD} \approx 18$ MHz) is maintained between the robust qubit states and the non-qubit states, successfully mitigating the effects of external magnetic noise fluctuations.

Replicating and advancing this breakthrough in robust quantum systems requires access to state-of-the-art diamond materials and advanced fabrication techniques. 6CCVD is uniquely positioned to supply the foundational materials and engineering support necessary for next-generation quantum sensing and computation.

To achieve the high $T_{2}$ performance demonstrated, the core material must minimize crystal defects and strain that cause inhomogeneous broadening and limit coherence.

6CCVD Material RecommendationGradeKey Capability Connection
Electronic Grade Single Crystal Diamond (SCD)Quantum/OpticalRequired for ultra-low concentration of substitutional nitrogen ([N] < 1 ppb) to ensure maximum NV center stability and initial $T_{2}^{*}$.
High-Purity SCD SubstratesLow-StrainMinimal birefringence and internal stress, crucial for maintaining the precise energy level separations (Zeeman splitting) required for off-resonant driving.
Custom NV CreationEngineering ServiceWhile NV creation is typically done post-growth (implantation/annealing), 6CCVD ensures the precursor material quality (low [N]) is optimal for high-fidelity NV defect creation and controlled spin manipulation.

NV-center experiments, particularly those involving microwave manipulation, require precise integration of the diamond substrate with external hardware.

  • Custom Dimensions: 6CCVD supplies inch-sized plates/wafers (up to 125mm PCD) and custom SCD slices, allowing researchers to choose optimal geometries for their microwave transmission lines (e.g., CPW structures).
  • Thickness Control: We offer SCD thickness control from 0.1 ”m up to 500 ”m, critical for optimizing microwave field coupling and minimizing absorption losses in sensing applications.
  • Advanced Metalization Services: The implementation of the driving fields often requires fabrication of microwave structures directly onto the diamond. 6CCVD provides in-house metalization using a wide range of materials, including: Ti/Pt/Au, Ti/W/Cu, or custom stacks, tailored for specific microwave frequencies ($\sim 17-23$ GHz in this case).
  • Surface Preparation: Achieving high-fidelity optical and microwave coupling requires atomically flat surfaces. Our advanced polishing capabilities deliver Ra < 1 nm (SCD), ensuring minimal surface scattering losses for optical initialization and readout.

The robust qubit scheme requires precise parameter optimization ($\Delta_{1} / \Delta_{2}$ ratio and $\Omega$). Success hinges on the quality and consistency of the host diamond.

6CCVD’s in-house PhD engineering team specializes in diamond material physics and defect engineering. We provide dedicated assistance with material selection for similar NV-center based Quantum Sensing or Quantum Information Processing projects, advising on optimal nitrogen concentration, crystallographic orientation, and surface termination to maximize qubit performance.

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

View Original Abstract

Abstract We present a new method of constructing a fully robust qubit in a three-level system. By the application of continuous driving fields, robustness to both external and controller noise is achieved. Specifically, magnetic noise and power fluctuations do not operate within the robust qubit subspace. Whereas all the continuous driving based constructions of such a fully robust qubit considered so far have required at least four levels, we show that in fact only three levels are necessary. This paves the way for simple constructions of a fully robust qubit in many atomic and solid state systems that are controlled by either microwave or optical fields. We focus on the NV-center in diamond and analyze the implementation of the scheme, by utilizing the electronic spin sub-levels of its ground state. In current state-of-the-art experimental setups the scheme leads to improvement of more than two orders of magnitude in coherence time, pushing it towards the lifetime limit. We show how the fully robust qubit can be used to implement quantum sensing, and in particular, the sensing of high frequency signals.