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Environmental noise spectroscopy with qubits subjected to dynamical decoupling

MetadataDetails
Publication Date2017-06-01
JournalJournal of Physics Condensed Matter
AuthorsP SzaƄkowski, G Ramon, J. Krzywda, D. Kwiatkowski, Ɓ. CywiƄski
InstitutionsUniversity of Warsaw, Santa Clara University
Citations109
AnalysisFull AI Review Included

Technical Documentation & Analysis: Environmental Noise Spectroscopy using MPCVD Diamond

Section titled “Technical Documentation & Analysis: Environmental Noise Spectroscopy using MPCVD Diamond”

This research paper details the critical technique of Dynamical Decoupling (DD)-based Noise Spectroscopy (DDNS), which utilizes quantum systems (qubits) as highly sensitive sensors to characterize their nanoscale environments.

  • Core Application: DDNS is essential for reconstructing the Power Spectral Density (PSD), $S(\omega)$, of environmental noise, crucial for advancing quantum computing and high-resolution sensing.
  • Platform Focus: Nitrogen-Vacancy (NV) centers in diamond are highlighted as the most prominent solid-state platform for this application, enabling nanoscale Nuclear Magnetic Resonance (NMR) and magnetic sensing.
  • Methodology: DD sequences (such as Carr-Purcell, PDD, and UDD) are applied to the qubit, acting as frequency-domain filters to suppress decoherence and isolate specific noise frequencies.
  • Material Requirement: Achieving long coherence times ($T_2$) and reliable noise reconstruction requires ultra-high-purity, low-defect Single Crystal Diamond (SCD) substrates to minimize intrinsic spin bath noise.
  • Noise Analysis: The study examines the applicability of the Gaussian noise approximation, demonstrating that non-Gaussian noise (like Random Telegraph Noise, RTN) can be effectively “Gaussianized” in the weak-coupling or large-ensemble limit, validating the DDNS method.
  • 6CCVD Value Proposition: 6CCVD provides the necessary high-quality, custom-engineered MPCVD SCD substrates and metalization capabilities required to replicate and extend this cutting-edge quantum sensing research.

The following hard data points and parameters are extracted from the analysis of DDNS applied to solid-state qubits, particularly NV centers in diamond.

ParameterValueUnitContext
Qubit PlatformNV CenterDiamondPrimary solid-state spin qubit discussed
Decoherence MechanismPure DephasingN/AAssumed mechanism ($T_1 \gg T_2$)
Noise Spectrum Reconstruction$S(\omega)$N/APower Spectral Density (PSD)
DD Sequence TypesCP, PDD, UDDN/AUsed for frequency-domain filtering
Filter Function Dependence$F(\omega T)/\omega^{2}$N/ADetermines noise suppression profile
Characteristic Frequency ($\omega_p$)$\pi/\tau$ or $2\pi/T$rad/sDetermined by interpulse time ($\tau$)
Example Interpulse Time ($\tau_{32}$)$4 \times 10^{-4}$secondsUsed in spectral reconstruction examples
Low-Frequency Noise Suppression (CP)$\omega^{4}$N/AStrong suppression for Carr-Purcell sequences
Low-Frequency Noise Suppression (UDD)$\omega^{2n+2}$N/AUniversal DD (UDD) for $n$ pulses
RTN Switching Rate ($\gamma$)0.1 to 5$\mu\text{eV}$Example non-Gaussian noise source
SCD Material RequirementLow NitrogenN/AEssential for minimizing intrinsic spin bath noise

The DDNS technique relies on precise control over the qubit and a detailed understanding of the noise environment. The core steps are:

  1. Qubit Selection and Isolation: Utilizing solid-state qubits (e.g., NV centers in diamond) where the system-environment coupling can be approximated as pure longitudinal dephasing, allowing $T_1$ (energy relaxation) to be neglected relative to $T_2$ (coherence time).
  2. Pulse Sequence Design: Applying sequences of instantaneous $\pi$ pulses (DD sequences) at specific intervals ($\tau$) to the qubit. Common sequences include Spin Echo (SE), Carr-Purcell (CP), and Periodic DD (PDD).
  3. Frequency Filtering: The DD sequence generates a time-domain filter function, $f_T(t)$, which translates in the frequency domain to a filter $|f_T(\omega)|^2$. This filter suppresses noise at low frequencies (long timescales) and creates sharp pass-bands (frequency comb) at the characteristic frequency $\omega_p = \pi/\tau$ and its odd harmonics.
  4. Coherence Measurement: Measuring the qubit coherence function, $W(T)$, as a function of total evolution time $T$ and pulse number $n$. For Gaussian noise, $W(T) = e^{-\chi(T)}$, where $\chi(T)$ is the attenuation factor.
  5. Spectral Density Reconstruction: Relating the measured attenuation factor $\chi(T)$ to the noise spectrum $S(\omega)$ via the integral $\chi(T) \propto \int d\omega |f_T(\omega)|^2 S(\omega)$. By varying the pulse spacing $\tau$ (and thus $\omega_p$), a system of linear equations is generated to reconstruct $S(\omega)$ at discrete frequencies.
  6. Non-Gaussian Analysis: Assessing the validity of the Gaussian approximation by comparing the second-order cumulant ($\chi_2$) to higher-order cumulants ($\chi_4$), particularly important when dealing with localized fluctuators (e.g., RTN).

6CCVD is uniquely positioned to supply the advanced diamond materials and engineering services required for high-fidelity DDNS experiments, particularly those involving NV centers and other solid-state qubits.

To replicate or extend the high-coherence NV center research discussed, researchers require diamond with exceptional purity and controlled defect density.

  • Optical Grade Single Crystal Diamond (SCD): This material is essential. 6CCVD provides low-nitrogen, high-purity SCD to maximize the coherence time ($T_2$) of the NV centers by minimizing the intrinsic nuclear and electronic spin bath noise floor.
  • Boron-Doped Diamond (BDD): For electrochemical or sensing applications requiring conductive diamond electrodes, 6CCVD offers custom BDD films, which can also be used as substrates for integrated quantum devices.

The paper emphasizes nanoscale sensing and the need for precise control structures (gates, microwave delivery). 6CCVD’s custom fabrication capabilities directly address these requirements:

Requirement from Research6CCVD Custom CapabilitySpecification
Substrate Size/ThicknessCustom Plates/WafersSCD: 0.1”m to 500”m thickness
Large Area PCDUp to 125mm diameter
Surface QualityUltra-Low Roughness PolishingRa < 1nm (SCD), Ra < 5nm (PCD)
Qubit Control IntegrationCustom MetalizationAu, Pt, Pd, Ti, W, Cu (Internal capability)
Substrate EngineeringThick SubstratesUp to 10mm thickness

The complexity of DDNS, particularly when dealing with non-Gaussian noise and multi-qubit cross-correlation spectroscopy (Section V C), necessitates expert material consultation.

  • Material Optimization: 6CCVD’s in-house PhD material science team assists researchers in optimizing diamond growth parameters (e.g., controlled nitrogen incorporation) to achieve the precise NV density and quality required for advanced Quantum Sensing and Noise Spectroscopy projects.
  • Noise Floor Management: We provide consultation on material selection and processing to ensure the lowest possible intrinsic noise floor, crucial for sensitive measurements like nanoscale NMR imaging.
  • Global Logistics: We offer reliable global shipping (DDU default, DDP available) to ensure timely delivery of custom materials worldwide.

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

View Original Abstract

A qubit subjected to pure dephasing due to classical Gaussian noise can be turned into a spectrometer of this noise by utilizing its readout under properly chosen dynamical decoupling (DD) sequences to reconstruct the power spectral density of the noise. We review the theory behind this DD-based noise spectroscopy technique, paying special attention to issues that arise when the environmental noise is non-Gaussian and/or it has truly quantum properties. While we focus on the theoretical basis of the method, we connect the discussed concepts with specific experiments, and provide an overview of environmental noise models relevant for solid-state based qubits, including quantum-dot based spin qubits, superconducting qubits, and NV centers in diamond.