Verification of single-photon path entanglement using a nitrogen vacancy center
At a Glance
Section titled âAt a Glanceâ| Metadata | Details |
|---|---|
| Publication Date | 2024-11-13 |
| Journal | Applied Optics |
| Authors | Alice I. Smith, Christine Steenkamp, Mark Tame |
| Institutions | Stellenbosch University, National Institute for Theoretical Physics |
| Citations | 2 |
| Analysis | Full AI Review Included |
Verification of Single-Photon Path Entanglement using an NV Center
Section titled âVerification of Single-Photon Path Entanglement using an NV CenterâExecutive Summary
Section titled âExecutive SummaryâThis research successfully demonstrates the generation and verification of single-photon path entanglement using a solid-state Nitrogen Vacancy (NV) center in a nanodiamond, offering a simplified, room-temperature platform for quantum photonics.
- Solid-State Advantage: Path entanglement was generated using a stable, room-temperature NV0 center in a nanodiamond, replacing complex, pulsed atomic ensembles (e.g., Cesium atoms) used in prior work.
- Simplified Excitation: The experiment utilized Continuous Wave (CW) laser excitation (532 nm) combined with a novel âtime-windowâ method for state generation, eliminating the need for a pulsed laser source.
- High Source Quality: The NV center was confirmed as a high-quality single-photon emitter, characterized by a second-order correlation g(2)(0) of 0.173 ± 0.039.
- High Coherence: The single photon exhibited high self-coherence, measured by a mean visibility (V) of 0.9329 ± 0.0069 (93.29%) in the Mach-Zehnder interferometer setup.
- Entanglement Verification: The presence of entanglement was verified using the Normalized Concurrence (CN), achieving a maximum value of 0.44 ± 0.07 at the minimum 2 ns time window.
- Quantum-Classical Transition: The study successfully observed the transition from quantum (entangled) to classical (non-entangled) behavior as the state-generation time window was increased, causing CN to decay toward zero.
Technical Specifications
Section titled âTechnical Specificationsâ| Parameter | Value | Unit | Context |
|---|---|---|---|
| NV Center Type | NV0 | - | Neutral Nitrogen Vacancy defect. |
| Host Material | Nanodiamond | - | Average 40 nm diameter. |
| Excitation Source | CW 532 | nm | Continuous Wave laser. |
| Pump Power | ~100 | ”W | Excitation power used for the sample. |
| Zero-Phonon Line (ZPL) | 575 | nm | Characteristic emission wavelength for NV0. |
| Peak Emission Wavelength | ~655 | nm | Room temperature peak fluorescence. |
| Second-Order Correlation (g(2)(0)) | 0.173 ± 0.039 | - | Confirms single-photon emission (less than 0.5). |
| Mean Visibility (V) | 0.9329 ± 0.0069 | - | Self-coherence of the single photon (93.29%). |
| Maximum Normalized Concurrence (CN) | 0.44 ± 0.07 | - | Measure of entanglement (at 2 ns window). |
| State Generation Window (ÎŽt) Range | 2 to 100 | ns | Range tested for entanglement generation. |
| Decay Constant (Îł1) | 0.035 | ns-1 | Obtained from g(2) fit model. |
| Lumped Detection Efficiency (ηD) | 0.0402 ± 0.0069 | - | Efficiency from generation stage output to detectors. |
| Confocal Lateral Resolution (dra) | ~0.5 | ”m | Detected collection area size. |
Key Methodologies
Section titled âKey MethodologiesâThe experiment combined standard confocal microscopy techniques with specialized quantum optics components for state generation and analysis.
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Sample Preparation and Excitation:
- Nanodiamonds (40 nm average diameter) were spin-coated onto a coverslip.
- A laser-scanning confocal microscope (Section A) using a 100x oil-immersion objective (NA = 1.3) was employed for excitation and collection.
- Excitation was performed using a CW 532 nm laser at approximately 100 ”W.
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NV Center Characterization:
- Fluorescence scans located potential NV centers.
- Second-order correlation (g(2)) measurements confirmed the single-photon emission regime (g(2)(0) = 0.173).
- Spectrum analysis confirmed the emitter type as NV0, based on the ZPL at 575 nm and the room-temperature peak at 655 nm.
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State Generation using CW and Time-Window Method:
- The single photon was input into a generation stage (Section C) consisting of a non-polarizing beamsplitter to create the path-entangled state: |Κ> = (1/â2) (|0>1 |1>2 + eiÏ |1>1 |0>2).
- A novel âtime-windowâ (ÎŽt) method (2 ns minimum) was used to define a state-generation period, replacing the trigger signal from pulsed lasers.
- Photon probabilities (p0, p1, p2) were measured within this window to quantify contamination (yc).
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Entanglement Analysis and Verification:
- The analysis stage (Section D) completed a Mach-Zehnder interferometer.
- Path-to-polarization tagging was implemented using a HWP and PBS to allow interference measurement via polarization detection (DH and DV detectors).
- Visibility Measurement: Interference fringes were measured by rotating a motorized HWP, yielding V = 0.9329.
- Concurrence Calculation: The Normalized Concurrence (CN) was calculated using the measured visibility (V) and the degree of contamination (yc), confirming CN > 0 for entanglement.
Commercial Applications
Section titled âCommercial ApplicationsâThe successful generation of path entanglement using a stable, room-temperature solid-state emitter validates key technologies for future quantum systems, particularly those requiring integrated or robust components.
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Quantum Communication Networks:
- Path-entangled single photons are a fundamental resource for Quantum Key Distribution (QKD) and quantum communication protocols (e.g., quantum teleportation, dense coding).
- The use of solid-state NV emitters facilitates the creation of stable, scalable quantum communication links and networks.
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Integrated Quantum Photonics:
- The methodology extends to other solid-state emitters (e.g., quantum dots) and supports the development of on-chip quantum circuits.
- Future work aims to increase the number of paths and utilize entanglement directly on-chip, crucial for scalable quantum processors.
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Quantum Sensing and Metrology:
- NV centers are established platforms for high-precision quantum sensing (e.g., magnetometry).
- Path entanglement can enhance precision in quantum metrology applications, including very-long-baseline interferometry for astronomy and geodesy.
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Robust Quantum Hardware:
- Operating the single-photon source at room temperature simplifies engineering requirements, reducing the need for complex cryogenic cooling systems typically associated with high-coherence quantum systems.
View Original Abstract
Path entanglement is an essential resource for photonic quantum information processing, including in quantum computing, quantum communication, and quantum sensing. In this work, we experimentally study the generation and verification of bipartite path-entangled states using single photons produced by a nitrogen vacancy center within a nanodiamond. We perform a range of measurements to characterize the photons being generated and verify the presence of path entanglement. The experiment is performed using continuous-wave laser excitation and a novel, to our knowledge, state-generation âtime-windowâ method. This approach to path entanglement verification is different from previous work as it does not make use of a pulsed laser excitation source.
Tech Support
Section titled âTech SupportâOriginal Source
Section titled âOriginal SourceâReferences
Section titled âReferencesâ- 2010 - Quantum Computation and Quantum Information