研究目的
Investigating the ionization and recombination dynamics of negatively charged and neutral nitrogen vacancy (NV) centers in diamond under green and infrared (IR) excitation to develop a quantitative model that explains experimental data and enhances the initialization fidelity of shallow NVs to the negatively charged state.
研究成果
The study provides a comprehensive quantitative model for NV center photodynamics under green and IR excitation, reconciling previous experimental discrepancies. Key differences between bulk and shallow NVs were identified, with shallow NVs showing enhanced ionization rates likely due to surface charge traps. An optimized two-color initialization procedure was developed to increase the NV- population in shallow NVs by up to 25%, offering improvements for applications in quantum sensing and information processing. Future work could explore fundamental internal dynamics and rates not fully resolved.
研究不足
The model does not fully explain highly nonlinear regimes. There are uncertainties in extracted rates due to variations between different NVs and assumptions in the model, such as no losses at the diamond interface and diffraction-limited beam focus. The study is limited to specific laser wavelengths (532 nm and 1064 nm) and may not generalize to other conditions.
1:Experimental Design and Method Selection:
A home-built confocal microscope was used to study NV centers under continuous wave green (532 nm) and IR (1064 nm) laser excitation. The methodology involved steady-state and time-resolved fluorescence measurements to analyze charge-state dynamics, with a rate equation model developed to describe the photodynamic processes.
2:Sample Selection and Data Sources:
Single shallow NVs were measured in a high-purity chemical vapor deposition (CVD) diamond sample (Element Six electronic grade, implanted with N15 and annealed) and bulk NVs in a high-pressure high-temperature (HPHT) sample (Element Six). Data were collected using fluorescence levels filtered for NV- and NV0 states.
3:List of Experimental Equipment and Materials:
Lasers: CNI MGL-III-532 100 mW (532 nm), II-VI SUWTECH DPIR 2200 (1064 nm). Modulators: Gooch and Housego AOMO 3080-
4:Objective:
1 Nikon Plan Apochromat 100X Oil Lambda NA
5:45 WD 13 mm. Detector:
Excelitas SPCM-700-13-FC single-photon counter. Filters: Semrock NF01-532U-25, Semrock FF01-736/128-25, Semrock FF01-600/52-
6:Samples:
Element Six CVD and HPHT diamonds.
7:Experimental Procedures and Operational Workflow:
The beam was focused to a diffraction-limited spot using an oil immersion objective. Fluorescence was collected and directed to the single-photon counter. Pulse sequences involved turning IR laser on and off while green laser was continuous, with measurements of fluorescence dynamics over time. Data were analyzed to extract ionization and recombination rates.
8:Data Analysis Methods:
Numerical optimization using ODE45 in MATLAB to solve rate equations based on an 8-level energy diagram. Cross sections were extracted from fits to experimental data using derived equations for quasi-steady-state populations.
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Laser
MGL-III-532
CNI
Provides green (532 nm) continuous wave excitation for NV centers.
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Acousto-Optic Modulator
AOMO 3080-125
Gooch and Housego
Modulates the laser beams for pulsed excitation sequences.
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Single-Photon Counter
SPCM-700-13-FC
Excelitas
Detects and counts fluorescence photons from NV centers.
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Filter
NF01-532U-25
Semrock
Filters out green laser reflection.
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Filter
FF01-736/128-25
Semrock
Selects fluorescence for specific charge states (e.g., NV- or NV0).
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Filter
FF01-600/52-25
Semrock
Selects fluorescence for specific charge states (e.g., NV- or NV0).
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Laser
DPIR 2200
II-VI SUWTECH
Provides infrared (1064 nm) continuous wave excitation for NV centers.
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Objective
Plan Apochromat 100X Oil Lambda
Nikon
Focuses the laser beams into a diffraction-limited spot and collects fluorescence.
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Diamond Sample
Electronic Grade
Element Six
Substrate containing nitrogen vacancy centers for experimentation.
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