Excited-State Lifetime of NV Centers for All-Optical Magnetic Field Sensing
At a Glance
Section titled “At a Glance”| Metadata | Details |
|---|---|
| Publication Date | 2024-03-25 |
| Journal | Sensors |
| Authors | Ludwig Horsthemke, Jens Pogorzelski, Dennis Stiegekötter, Frederik Hoffmann, Lutz Langguth |
| Institutions | Quantum Design (Germany), FH Münster |
| Citations | 9 |
| Analysis | Full AI Review Included |
Technical Documentation & Analysis: Excited-State Lifetime of NV Centers for All-Optical Magnetic Field Sensing
Section titled “Technical Documentation & Analysis: Excited-State Lifetime of NV Centers for All-Optical Magnetic Field Sensing”This document analyzes the research paper “Excited-State Lifetime of NV Centers for All-Optical Magnetic Field Sensing” (Sensors 2024, 24, 2093) to provide technical specifications and align the findings with 6CCVD’s advanced MPCVD diamond capabilities.
Executive Summary
Section titled “Executive Summary”- Robust Sensing Mechanism: The research successfully demonstrates robust, all-optical magnetic field sensing by utilizing the excited-state fluorescence lifetime (a non-intensity quantity) of high-density Nitrogen-Vacancy (NV) microdiamonds.
- High Immunity Achieved: The phase-based detection method, measured at an optimal modulation frequency of 13 MHz, yielded a 100-times higher immunity to optical path fluctuations (e.g., laser noise, fiber movement) compared to traditional intensity-based approaches.
- Material Characteristics: The high-NV-density microdiamond powder exhibited bi-exponential fluorescence decay (6.13 ns and 14.54 ns at B=0), with the larger decay time showing a magnetic contrast of 15.2%.
- Performance Metrics: A realized noise floor of 20 µT/√Hz was achieved, approaching the calculated shot-noise-limited sensitivity of 0.95 µT/√Hz.
- Industrial Applicability: The fiber-coupled, microwave (MW)-free setup is compact and operates in a high magnetic field range (10-40 mT), establishing a strong basis for industrial quantum sensing applications where galvanic connections are undesirable.
- 6CCVD Relevance: The success of this method relies critically on high-quality, high-NV-density diamond material, a core specialty of 6CCVD’s MPCVD growth and processing capabilities.
Technical Specifications
Section titled “Technical Specifications”| Parameter | Value | Unit | Context |
|---|---|---|---|
| Material Type | High-NV-density | Powder | µm-sized microdiamonds |
| Fluorescence Decay (Short) | 6.13 | ns | Bi-exponential component (τ2,1) at B=0 |
| Fluorescence Decay (Long) | 14.54 | ns | Bi-exponential component (τ2,2) at B=0 |
| Magnetic Contrast (Lifetime) | 15.2 | % | Contrast observed in the larger decay time (τ2,2) |
| Optimal Modulation Frequency | 13 | MHz | Frequency yielding maximum phase contrast |
| Maximum Phase Contrast | 5.8 | ° | Phase shift at 13 MHz |
| Excitation Wavelength | 520 | nm | Laser diode used for frequency domain sensing |
| Modulation Frequency Range | Up to 100 | MHz | Frequency sweep range |
| Applied Magnetic Field Range | 0 to ~120 | mT | Range tested in the experiment |
| Realized Noise Floor (Phase) | 20 | µT/√Hz | Sensitivity achieved above 1 Hz |
| Shot-Noise-Limited Sensitivity | 0.95 | µT/√Hz | Theoretical limit for phase-based detection |
| Immunity Improvement | 100 | times | Phase-based vs. intensity-based approach |
| Fiber Core Diameter | 105 | µm | Multimode fiber used for sensor head |
Key Methodologies
Section titled “Key Methodologies”The experiment utilized two primary measurement techniques: Time-Correlated Single-Photon Counting (TCSPC) for material characterization and Frequency Domain Measurement (FDM) for robust sensing.
- Material Preparation: High-NV-density microdiamond powder was fixed to the tip of a 105 µm core optical fiber using glue to create a compact, fiber-coupled sensor head.
- TCSPC Characterization: A 515 nm ps-Laser was used to excite the sample. Fluorescence decay histograms were acquired and analyzed using Non-Linear Least Squares (NLLS) fitting, confirming a bi-exponential decay behavior.
- Excitation Modulation: A 520 nm laser diode was driven by a constant current source and modulated by an AC-coupled Radio Frequency (RF) amplifier at frequencies up to 100 MHz.
- Frequency Domain Acquisition: The fluorescence signal was collected through the same fiber, passed through a long-pass filter, and detected by a Si-photodiode/Trans-Impedance Amplifier (TIA).
- Signal Processing: A Vector Network Analyzer (VNA) or a Lock-In Amplifier (LIA) was used to record the magnitude and phase of the fluorescence signal relative to the excitation frequency.
- Reference Calibration: Measurements were normalized to the response at B = 0 mT to isolate the magnetic field-dependent change in fluorescence decay dynamics.
- Phase-Based Sensing: The LIA was specifically operated at 13 MHz (the frequency of maximum phase contrast) to measure the phase shift (∠Hr), providing inherent immunity to laser intensity noise and optical path fluctuations.
6CCVD Solutions & Capabilities
Section titled “6CCVD Solutions & Capabilities”The successful implementation of this all-optical magnetometry technique relies on high-quality, high-NV-density diamond material and precise integration capabilities. 6CCVD is uniquely positioned to supply the necessary materials and engineering support to replicate and advance this research toward industrial deployment.
| Research Requirement / Challenge | 6CCVD Solution & Capability | Technical Advantage for Quantum Sensing |
|---|---|---|
| High-NV Concentration Diamond | High-Nitrogen Polycrystalline Diamond (PCD) Wafers. We specialize in MPCVD growth with controlled nitrogen incorporation to maximize NV ensemble density. | Ensures high fluorescence signal strength (high count rate) necessary to achieve the reported shot-noise-limited sensitivity of 0.95 µT/√Hz. |
| Custom Sensor Geometry | Custom Dimensions & Laser Cutting. We provide PCD plates up to 125 mm and SCD plates in thicknesses ranging from 0.1 µm to 500 µm, cut to precise dimensions for fiber integration. | Enables the fabrication of compact, reproducible sensor heads optimized for coupling to 105 µm core fibers or micro-optics, moving beyond powder/glue methods. |
| Surface Quality for Optical Coupling | Ultra-Low Roughness Polishing. We offer polishing services achieving Ra < 5 nm for inch-size PCD and Ra < 1 nm for SCD. | Minimizes scattering and reflection losses at the diamond-fiber interface, maximizing the efficiency of both 520 nm excitation and fluorescence collection. |
| Robust Integration & Heat Management | Custom Metalization Services. We provide in-house deposition of standard metal stacks (e.g., Ti/Pt/Au, W/Cu) for robust bonding, thermal management, or creating electrical contacts. | Ensures reliable, high-adhesion interfaces for permanent integration into industrial probes, mitigating thermal drift that could affect optical alignment. |
| Replication and Optimization | Expert Engineering Support. Our in-house PhD team assists with material selection, NV creation recipes (e.g., optimizing annealing parameters), and thickness selection for specific decay dynamics. | Accelerates R&D for engineers seeking to tune the bi-exponential decay components or explore alternative materials like Boron-Doped Diamond (BDD) for electrochemistry applications. |
| Global Supply Chain | Global Shipping (DDU/DDP). We ensure reliable, worldwide delivery of sensitive diamond materials. | Guarantees timely access to critical quantum materials, supporting international research collaborations and industrial prototyping. |
For custom specifications or material consultation, visit 6ccvd.com or contact our engineering team directly.
View Original Abstract
We investigate the magnetic field-dependent fluorescence lifetime of microdiamond powder containing a high density of nitrogen-vacancy centers. This constitutes a non-intensity quantity for robust, all-optical magnetic field sensing. We propose a fiber-based setup in which the excitation intensity is modulated in a frequency range up to 100MHz. The change in magnitude and phase of the fluorescence relative to B=0 is recorded where the phase shows a maximum in magnetic contrast of 5.8∘ at 13MHz. A lock-in amplifier-based setup utilizing the change in phase at this frequency shows a 100 times higher immunity to fluctuations in the optical path compared to the intensity-based approach. A noise floor of 20μT/Hz and a shot-noise-limited sensitivity of 0.95μT/Hz were determined.
Tech Support
Section titled “Tech Support”Original Source
Section titled “Original Source”References
Section titled “References”- 2020 - Sensitivity optimization for NV-diamond magnetometry [Crossref]
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- 2017 - Scanning diamond NV center probes compatible with conventional AFM technology [Crossref]
- 2009 - Time-averaging within the excited state of the nitrogen-vacancy centre in diamond [Crossref]
- 2020 - Isotropic Scalar Quantum Sensing of Magnetic Fields for Industrial Application [Crossref]
- 2014 - Fiber-optic magnetic-field imaging [Crossref]
- 2021 - All-optical and microwave-free detection of Meissner screening using nitrogen-vacancy centers in diamond [Crossref]
- 2015 - Low-field feature in the magnetic spectra of N-V centers in diamond [Crossref]
- 2016 - Microwave-free magnetometry with nitrogen-vacancy centers in diamond [Crossref]