Tin-Vacancy Centers in Diamond for Quantum Network
At a Glance
Section titled âAt a Glanceâ| Metadata | Details |
|---|---|
| Publication Date | 2021-01-01 |
| Journal | The Review of Laser Engineering |
| Authors | Takayuki Iwasaki |
| Institutions | Tokyo Institute of Technology |
| Analysis | Full AI Review Included |
Technical Documentation: SnV Centers in Diamond for Quantum Networks
Section titled âTechnical Documentation: SnV Centers in Diamond for Quantum NetworksâThis document analyzes the research on Tin-Vacancy (SnV) centers in diamond, highlighting the material requirements necessary to advance this promising quantum emitter technology. 6CCVD specializes in providing the high-purity, isotopically enriched, and custom-dimensioned MPCVD diamond required for successful replication and extension of this research.
Executive Summary
Section titled âExecutive SummaryâThe research confirms the potential of SnV centers as superior quantum emitters for quantum network applications, overcoming limitations found in SiV and GeV centers.
- Superior Emitter: SnV centers exhibit a sharp Zero Phonon Line (ZPL) at 619 nm and high fluorescence intensity, making them excellent single-photon sources.
- Enhanced Spin Properties: The SnV center possesses a large ground state splitting ($\Delta G_S$) of approximately 850 GHz, significantly higher than SiV/GeV, which is crucial for suppressing phonon-induced decoherence at Kelvin temperatures.
- Coherence Achievement: Initial spin dephasing time (T2*) of 540 ns was measured at 2.9 K, demonstrating superior performance compared to other Group-IV centers at similar temperatures.
- Material Criticality: Achieving long spin coherence times (T2) requires the use of isotopically enriched 12C diamond to minimize interaction with 13C nuclear spins.
- Processing Requirement: High-quality SnV formation necessitates extreme thermal stability, requiring annealing temperatures of 2000 °C or higher.
- Future Development: Success hinges on advanced spin control techniques (CPMG, XY8) and precise control over multiple emitters (wavelength tuning via strain/devices) to achieve Hong-Ou-Mandel (HOM) interference.
Technical Specifications
Section titled âTechnical Specificationsâ| Parameter | Value | Unit | Context |
|---|---|---|---|
| Zero Phonon Line (ZPL) Wavelength | 619 | nm | Room temperature Photoluminescence (PL) spectrum |
| Required Annealing Temperature | > 2000 | °C | Necessary for high-quality SnV center formation |
| Ground State Splitting ($\Delta G_S$) | ~850 | GHz | Determined via low-temperature PL fine structure |
| Fourier-Limited Linewidth | ~18 | MHz | Derived from excited state lifetime |
| Initial Spin Dephasing Time (T2*) | 540 | ns | Measured using CW-ODMR at 2.9 K |
| Target Spin Coherence Time (T2) | Microseconds to Milliseconds | N/A | Goal for robust quantum memory applications |
| Required 13C Concentration | Low (Isotopically Enriched) | % | To suppress nuclear spin decoherence effects |
Key Methodologies
Section titled âKey MethodologiesâThe research relies on advanced material synthesis and precise quantum measurement techniques:
- SnV Center Creation: Sn atoms are introduced into the diamond lattice, followed by high-temperature annealing (2000 °C or higher) to form high-quality SnV centers with D3d symmetry.
- Optical Characterization: Photoluminescence (PL) spectroscopy is used to confirm the ZPL at 619 nm and low-temperature PL is used to measure the fine structure and determine the large ground state splitting ($\Delta G_S$).
- Spin Measurement: Continuous Wave Optically Detected Magnetic Resonance (CW-ODMR) is employed to measure the initial spin dephasing time (T2*).
- Coherence Extension (Proposed): Pulsed microwave sequences, including Hahn Echo, Carr-Purcell-Meiboom-Gill (CPMG), and XY8 dynamic decoupling sequences, are proposed to extend the spin coherence time (T2).
- Wavelength Control: Techniques such as applying strain (via nanostructures or devices) or utilizing p-n junction structures are necessary to precisely tune and match the emission wavelength of separated SnV centers.
- Quantum Interference Testing: Hong-Ou-Mandel (HOM) interference experiments are required to verify the indistinguishability of photons emitted from spatially separated, identical SnV quantum emitters.
6CCVD Solutions & Capabilities
Section titled â6CCVD Solutions & Capabilitiesâ6CCVD provides the specialized MPCVD diamond materials and processing services essential for replicating and advancing SnV quantum emitter research, particularly focusing on material purity, thermal stability, and device integration.
Applicable Materials
Section titled âApplicable MaterialsâTo achieve the long spin coherence times (T2) required for quantum networks, the material must minimize decoherence sources.
| Material Specification | 6CCVD Offering | Application Context |
|---|---|---|
| Isotopically Enriched Single Crystal Diamond (SCD) | Ultra-high purity SCD with < 0.1% 13C concentration. | Essential for suppressing electron spin interaction with 13C nuclear spins, enabling T2 extension via dynamic decoupling sequences (CPMG/XY8). |
| High-Purity SCD Substrates | SCD substrates up to 10 mm thick, capable of withstanding extreme processing. | Required for supporting thin films during the critical high-temperature annealing step (> 2000 °C) necessary for SnV formation. |
| Optical Grade SCD Thin Films | SCD layers from 0.1 ”m to 500 ”m thick, polished to Ra < 1 nm. | Provides the low-defect host material necessary for high-fluorescence, Fourier-limited linewidth SnV centers, and facilitates nanophotonic device fabrication. |
Customization Potential
Section titled âCustomization PotentialâThe research explicitly calls for advanced device structures (e.g., p-n junctions) and nanostructure integration for strain control and wavelength tuning. 6CCVD offers comprehensive customization capabilities to meet these engineering demands.
| Research Requirement | 6CCVD Customization Service | Technical Benefit |
|---|---|---|
| Device Integration & Electrical Contacts | Custom Metalization: Deposition of Au, Pt, Pd, Ti, W, or Cu layers. | Enables reliable electrical injection, readout, and the fabrication of p-n junction devices for wavelength tuning and advanced control. |
| Nanostructure Fabrication | Ultra-Low Roughness Polishing: Ra < 1 nm (SCD) and Ra < 5 nm (PCD). | Ensures optimal surface quality for lithography, etching, and the creation of high-Q nanophotonic cavities and waveguides. |
| Unique Dimensions | Custom Dimensions: Plates/wafers up to 125 mm (PCD) or custom-cut SCD. | Supports scaling from fundamental research to integrated quantum circuits and large-scale device arrays. |
| Strain Engineering | Precision Thickness Control: SCD films grown to exact specifications (e.g., 5 ”m ± 0.1 ”m). | Critical for controlled strain application, which is necessary to match the ZPL wavelength of separated SnV emitters for HOM interference. |
Engineering Support
Section titled âEngineering Supportâ6CCVDâs in-house team of PhD material scientists and engineers are experts in MPCVD growth parameters, defect engineering, and post-processing stability.
- Material Selection Consultation: Our team assists researchers in selecting the optimal diamond grade (e.g., isotopic purity, nitrogen concentration) to maximize SnV yield and coherence time for specific Quantum Emitter and Quantum Network projects.
- Thermal Stability Analysis: We provide technical guidance on the thermal budget and material stability required for high-temperature annealing processes (> 2000 °C) without compromising the diamond substrate or thin film interface.
- Integration Expertise: Support is available for optimizing metalization recipes and surface preparation techniques crucial for creating robust electrical and photonic interfaces.
For custom specifications or material consultation, visit 6ccvd.com or contact our engineering team directly.
View Original Abstract
Quantum emitters in diamond are a promising candidate for quantum network applications. Here, we show basic properties of tin-vacancy (SnV) centers in diamond, which we recently discovered. The SnV center shows a sharp zero phonon line and a high fluorescence intensity. The SnV center has a possibility to have a long spin coherence time in the Kelvin temperature range, in contrast to other group-IV color centers, i.e. silicon-vacancy and germanium-vacancy centers. We discuss important experiments regarding spin and optical properties of the SnV quantum emitter for further development towards quantum network.