High-sensitivity spin-based electrometry with an ensemble of nitrogen-vacancy centers in diamond
At a Glance
Section titled âAt a Glanceâ| Metadata | Details |
|---|---|
| Publication Date | 2017-05-01 |
| Journal | DSpace@MIT (Massachusetts Institute of Technology) |
| Authors | Philip Hemmer, Edward H. Chen, Hannah Clevenson, Kerry A. Johnson, Linh Pham |
| Analysis | Full AI Review Included |
Technical Analysis and Documentation for Spin-Based Electrometry
Section titled âTechnical Analysis and Documentation for Spin-Based ElectrometryâExecutive Summary
Section titled âExecutive SummaryâThis documentation analyzes a breakthrough research paper demonstrating a high-sensitivity, solid-state electrometer utilizing an ensemble of Nitrogen-Vacancy (NV$^-$) centers in CVD diamond.
- Core Achievement: Demonstrated a spin-based, all-dielectric electrometer achieving shot-noise-limited sensitivities approaching 1 (V/cm)/âHz in the ultra-low frequency regime (0.05-10 Hz).
- Mechanism: Detection relies on the electric-field-induced Stark shift on the NV$^-$ ground state, measured via Optically Detected Magnetic Resonance (ODMR).
- Noise Mitigation: The method successfully separates temperature-induced noise (D parameter fluctuations) from electric-field fluctuations, allowing for highly stable measurements under ambient conditions.
- Material Requirements: The experiment utilized a 3.0 x 3.0 x 0.32 mmÂł diamond plate grown via Chemical Vapor Deposition (CVD) with low nitrogen concentration (~1 ppb NV$^-$ density).
- Future Potential: Theoretical projections show that utilizing high-density, low-strain SCD material could improve sensitivity to 6 x 10-3 (V/cm)/âHz, yielding a 200x performance enhancement over current results.
- Application: This technique is critical for miniaturized, highly localized electric field sensing in applications such as microelectronic diagnostics and in vitro biological studies, operating below the optical diffraction limit.
- 6CCVD Value: 6CCVD specializes in the custom, low-strain Single Crystal Diamond (SCD) material required to replicate this sensitivity and achieve the projected performance gains through controlled doping and precision metalization.
Technical Specifications
Section titled âTechnical Specificationsâ| Parameter | Value | Unit | Context |
|---|---|---|---|
| Diamond Plate Dimensions | 3.0 x 3.0 x 0.32 | mmÂł | Material used for ensemble NV$^-$ detection |
| Crystallographic Orientation | (100) | Face | Orientation used for electrode evaporation |
| Initial NV$^-$ Density | ~1 | ppb | Produced during CVD growth process |
| Measured Sensitivity (Shot-Noise Limited) | 1.0 ± 0.1 | (V/cm)/âHz | NV$^-$ ground state sensitivity |
| Projected Sensitivity (Optimized Material) | 6 x 10-3 | (V/cm)/âHz | Anticipated maximum sensitivity with high-density NV$^-$ |
| Operating Frequency Range | 0.05 - 10 | Hz | Demonstrated low-frequency operation |
| Dynamic Range | 20 | dB | Measured range of electrometer operation |
| Incident Laser Power | 1.8 | W | Power used to achieve maximum sensitivity |
| Laser Power Density (Saturation) | ~30 | ”W/”mÂČ | High power required to saturate NV$^-$ photoluminescence |
| Ground State Crystal-Field Splitting (D) | 2.8 | GHz | Key parameter used for ODMR temperature compensation |
| Ground State Transverse Field Sensitivity (dâ„) | 17 | Hz/(V/cm) | Required material characteristic for Stark shift sensing |
Key Methodologies
Section titled âKey MethodologiesâThe experiment utilized a comprehensive MPCVD diamond synthesis and integration workflow, demonstrating capabilities in both material control and high-speed readout.
- Material Growth and Preparation:
- CVD diamond plate (3.0 x 3.0 x 0.32 mmÂł) with (100) faces was synthesized, achieving a low NV$^-$ concentration (~1 ppb).
- Electrode Fabrication:
- Gold (Au) electrodes were custom-evaporated onto the two parallel (100) faces of the diamond plate to apply the necessary electric fields ($E$).
- Optical Excitation and Readout:
- A continuous-wave (CW) laser beam (~200 ”m diameter) was focused through the edge of the diamond plate to excite the NV$^-$ ensemble.
- Photoluminescence (PL) was collected by a lens setup and detected by a Silicon detector.
- Microwave (MW) Delivery:
- MW excitation was applied locally via an $\Omega$-shaped stripline patterned on a printed circuit board (PCB), allowing for ODMR measurements.
- Detection System Integration:
- A custom, home-built digital lock-in amplifier (LIA) system, utilizing a high-speed Field-Programmable Gate Array (FPGA) and Digital-to-Analog Converter (DAC), performed both waveform generation and signal readout.
- Noise Compensation:
- Electric-field fluctuations were distinguished from thermal fluctuations by simultaneously monitoring two strain/electric-field sensitive transitions (m$_{s}$ = ±0). The difference of these time traces isolated the electric-field signal, while the sum revealed the temperature fluctuations (due to the D parameter shift).
6CCVD Solutions & Capabilities
Section titled â6CCVD Solutions & Capabilitiesâ6CCVD is uniquely positioned to supply the advanced diamond material and fabrication services required to replicate this high-sensitivity electrometer and achieve the predicted 200x performance increase.
Applicable Materials & Optimization
Section titled âApplicable Materials & OptimizationâTo replicate and extend this research, 6CCVD recommends providing Optical Grade Single Crystal Diamond (SCD) engineered specifically for quantum sensing applications.
- High Purity, Controlled Doping: To achieve the projected sensitivity of 6 x 10-3 (V/cm)/âHz, researchers require SCD with a significantly higher density of NV$^-$ centers (up to 1000x denser than the 1 ppb material used). 6CCVD offers controlled nitrogen doping during the MPCVD growth process (or post-processing irradiation/annealing optimization) to achieve high, uniform NV ensemble densities (ppm range).
- Low Strain Requirement: High-sensitivity electrometry relies on long inhomogeneous coherence times ($T_{2}^{}$). Our Low-Strain MPCVD SCD material minimizes crystal defects and internal strain ($\Pi$), directly supporting longer $T_{2}^{}$ coherence and maximizing electrometer performance according to the shot-noise sensitivity equation (Eq. 4).
- Orientation: We routinely supply SCD wafers with precise (100) or (111) crystallographic orientations, ensuring optimal alignment for electrode deposition and electric field application relative to the NV axis.
Customization Potential for Replication & Scaling
Section titled âCustomization Potential for Replication & Scalingâ| Requirement from Paper | 6CCVD Custom Capability | Engineering Advantage |
|---|---|---|
| Custom Dimensions (3 x 3 x 0.32 mm³) | We provide plates/wafers in custom dimensions, replicating the exact size used or scaling up to 125 mm (PCD). SCD plates are available up to 500 ”m thickness. | Enables rapid prototyping and scaling to production volumes for compact sensor arrays. |
| Metalization Layers (Au Electrodes) | Full In-House Metalization Suite: We offer custom thin-film deposition including Au, Pt, Ti, Pd, W, and Cu. We can deposit the necessary Ti/Au or Ti/Pt/Au schemes for robust ohmic contact electrodes. | Eliminates the need for external cleanroom access, ensuring high-quality, repeatable electrode integration onto the diamond surface. |
| Surface Finish | Precision Polishing: SCD is polished to roughness Ra < 1nm, critical for optimal optical coupling efficiency and reducing scattering losses. | Enhances photon collection rate ($\Gamma$), which is a critical factor in achieving projected shot-noise limited sensitivity (Eq. 4). |
| Deep Etching/Structuring | Available internal laser cutting and deep reactive ion etching (DRIE) for creating waveguides or resonant structures. | Allows for future integration of optical patterning needed to increase photon collection efficiency (up to 100x improvement cited in the paper). |
Engineering Support
Section titled âEngineering Supportâ6CCVDâs in-house PhD material science team can assist researchers and technical engineers in optimizing the diamond recipe for similar Spin-Based Quantum Sensing projects. We offer consultation on:
- Selecting the ideal nitrogen concentration (ppb vs. ppm) to balance NV density and coherence properties ($T_{2}^{*}$).
- Specifying the appropriate crystal orientation for maximal transverse electric susceptibility ($k_{\perp}$).
- Designing robust metalization layouts compatible with high-power MW excitation and low-frequency DC bias voltage application.
For custom specifications or material consultation, visit 6ccvd.com or contact our engineering team directly.
View Original Abstract
We demonstrate a spin-based, all-dielectric electrometer based on an ensemble of nitrogen-vacancy (NV[superscript â]) defects in diamond. An applied electric field causes energy-level shifts symmetrically away from the NV[superscript â]âs degenerate triplet states via the Stark effect; this symmetry provides immunity to temperature fluctuations allowing for shot-noise-limited detection. Using an ensemble of NV[superscript â]s, we demonstrate shot-noise-limited sensitivities approaching 1 (V/cm)/âHz under ambient conditions, at low frequencies (<10 Hz), and over a large dynamic range (20 dB). A theoretical model for the ensemble of NV[superscript â]s fits well with measurements of the ground-state electric susceptibility parameter â©k[subscript â„]âȘ. Implications of spin-based, dielectric sensors for micron-scale electric-field sensing are discussed.
Tech Support
Section titled âTech SupportâOriginal Source
Section titled âOriginal Sourceâ- DOI: None