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Decoherence Control of Nitrogen-Vacancy Centers

MetadataDetails
Publication Date2017-09-14
JournalScientific Reports
AuthorsChao Lei, Shijie Peng, Chenyong Ju, Man‐Hong Yung, Jiangfeng Du
InstitutionsUniversity of Science and Technology of China, Southern University of Science and Technology
Citations17
AnalysisFull AI Review Included

Technical Documentation: Decoherence Control in Diamond NV Centers

Section titled “Technical Documentation: Decoherence Control in Diamond NV Centers”

This analysis addresses the research paper “Decoherence Control of Nitrogen-Vacancy Centers,” focusing on utilizing advanced diamond material properties and specialized engineering techniques to manipulate quantum coherence (T2) for simulating open quantum systems.


The following outline summarizes the core technical achievements and scientific value of the presented research, positioning 6CCVD’s role in enabling such advanced solid-state quantum experiments.

  • Core Achievement: Demonstration of external control over the decoherence time (T2) of Nitrogen-Vacancy (NV) centers in diamond, a necessary capability for simulating complex open quantum systems.
  • Methodology: A hybrid approach combining digital quantum simulation ingredients (Trotter decomposition) and analog control techniques (Dynamical Decoupling pulse sequences) to dynamically couple or decouple the NV center spin from its environment (spin bath).
  • Decoherence Tuning: The system-environment coupling strength is engineered using the external parameter $\lambda$ (for strengthening) and $\mu$ (for weakening), allowing T2 times to be tuned across a significant range (e.g., from ~5 ”s up to ~35 ”s).
  • Versatile Platform: The method is shown to be effective across two-level (qubit) and three-level (qudit) systems, with the capability to fine-tune the decoherence rate of individual off-diagonal elements in the density matrix.
  • Material Dependence: The successful operation relies fundamentally on high-quality diamond material with controllable impurity levels (13C nuclear spins and P1 electron spins) which constitute the environmental spin bath.
  • Relevance: This work establishes NV centers as a highly controllable platform for universal quantum computation and, critically, for benchmarking non-Markovian open quantum systems.

The following hard data points were extracted from the numerical simulations and experimental context described in the paper.

ParameterValueUnitContext
NV Zero-Field Splitting (D)2.87GHzIntrinsic NV Property
Static Magnetic Field (Bz)100GaussApplied along the [111] axis of the crystal
NV Resonance Frequency3.15GHzCalculated at the applied 100 Gauss field
Applied Microwave (MW) Amplitude1.717GaussUsed to drive spin transitions (swap gates)
MW Detuning1.9 x 106 / (1 + $\lambda$)HzFrequency offset used during simulation
Achieved Coherence Time (T2) Range~5 to ~35”sControllable via system coupling parameter $\lambda$
Target System3-Dimensional QuditN/ANV spin states
Noise Source 113C Nuclear SpinsN/AStationary Gaussian noise (dominant in ultra-pure diamond)
Noise Source 2P1 Electron SpinsN/AOrnstein-Uhlenbeck process (dominant in nitrogen-doped diamond)

The experiment uses a sophisticated sequence of laser and microwave pulses to manipulate the NV spin and control its coupling to the surrounding environment.

  1. System Preparation: The NV center is initialized into a desired spin state (typically the |0> state) using standard laser excitation techniques and subsequent microwave application.
  2. Hamiltonian Engineering (Rotating Frame): The static NV Hamiltonian ($H_{NV}$) is transformed using two sets of applied microwave pulses ($\omega_{1}, \omega_{2}$), which are tuned near resonance conditions ($\omega_{1} = D + \gamma B_{z}$, $\omega_{2} = D - \gamma B_{z}$) to create a controllable effective simulated Hamiltonian ($H_{S}$).
  3. Strengthening Decoherence (Trotter Decomposition):
    • The total system evolution is divided into small time slices ($\Delta t$).
    • During the slice, the system Hamiltonian ($H_{S}$) is temporarily turned off ($B_{1/2}=0$), allowing the system-environment interaction ($H_{SB}$) to evolve freely.
    • This technique effectively amplifies the system-environment coupling strength by a factor $(1 + \lambda)$, drastically reducing $T_{2}$ (Decoherence Strengthening).
  4. Weakening Decoherence (Dynamical Decoupling):
    • Swap gates ($\pi$ pulses, $\sigma_{x}$ rotation) are inserted during the evolution period.
    • By carefully controlling the timing ($t_{1}, t_{2}$) between these gates, the effective coupling to the environment ($H_{SB}$) is decreased or nearly eliminated, resulting in a large increase in T2 time.
  5. Fine-Tuning Qudit Decoherence: For the three-level system, specialized dual-channel decoupling sequences (using MW1 and MW2 at different frequencies) are applied to control the decoherence of individual off-diagonal coherence elements ($\rho_{12}, \rho_{13}, \rho_{23}$) independently.

Replicating or advancing this research requires diamond substrates of exceptional crystalline quality and precise control over environmental impurities. 6CCVD is an expert technical supplier providing the necessary materials and fabrication services.

Research Requirement (NV Platform)6CCVD Applicable Materials & ServicesTechnical Specification Relevance
Ultra-Pure Diamond SubstratesOptical Grade Single Crystal Diamond (SCD): Low concentration of Nitrogen (< 1 ppb or as specified).Required to minimize P1 electron spin noise, isolating the 13C spin bath for fundamental open system simulations (Fig. 1a, 1b). Allows for the longest possible intrinsic T2.
Engineered Spin BathCustom Nitrogen/Isotopic Doping: Controlled concentration of substitutional Nitrogen (P1 centers) or tailored 13C isotopic percentage.Essential for simulating open quantum systems where the environment (spin bath) is a dominant and necessary feature (Fig. 1c, 1d, Type I diamond).
Custom Dimensions/ScalabilitySCD/PCD Wafers and Plates: Custom dimensions up to 125 mm (PCD). Substrates up to 10 mm thickness.Provides scalable platforms for integrating quantum control circuitry and multi-qubit devices.
Precision Optical CouplingUltra-Polished SCD Surfaces: Achieved roughness Ra < 1 nm.Critical for high-fidelity laser initialization and readout, minimizing scatter loss and ensuring efficient collection of NV photoluminescence.
Microwave Control CircuitryCustom Metalization Services: In-house deposition of Au, Pt, Pd, Ti, W, Cu.Required for fabricating high-frequency coplanar waveguides (CPW) or microstrip lines directly on the diamond surface to deliver the necessary strong B1/2 microwave pulses (1.717 Gauss amplitude) used for $\pi$ pulses and swap gates.
Device IntegrationLaser Cutting & Shaping: Services for intricate geometries required for RF devices and coupling.Enables the production of precisely sized plates and custom geometries for high-stability mounting in cryogenic or room-temperature quantum setups.

6CCVD provides the foundational material science expertise necessary to control the defect density and purity—factors that determine the intrinsic noise environment (T2) of the NV center—which this research then exploits for advanced control.

Our in-house PhD team offers comprehensive engineering support to assist researchers and technical engineers in selecting the optimal diamond growth parameters (purity, doping, thickness) and fabrication path (polishing, metalization) required to replicate this decoherence control research or extend it to new quantum simulation projects.

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