Inverse-designed photon extractors for optically addressable defect qubits
At a Glance
Section titled âAt a Glanceâ| Metadata | Details |
|---|---|
| Publication Date | 2020-11-17 |
| Journal | Optica |
| Authors | Srivatsa Chakravarthi, Pengning Chao, Christian Pederson, Sean Molesky, Andrew Ivanov |
| Citations | 36 |
| Analysis | Full AI Review Included |
Technical Documentation & Analysis: Inverse-Designed Photon Extractors
Section titled âTechnical Documentation & Analysis: Inverse-Designed Photon ExtractorsâReference: Chakravarthi et al., âInverse-designed photon extractors for optically addressable defect qubits,â arXiv:2007.12344v3 (2020).
Executive Summary
Section titled âExecutive SummaryâThis research demonstrates a critical advancement in solid-state quantum technology by utilizing inverse-designed photonic structures to enhance the performance of near-surface Nitrogen-Vacancy (NV) centers in diamond.
- Core Achievement: Demonstrated a compact hybrid Gallium Phosphide (GaP)-on-Diamond planar dielectric structure achieving up to a 14-fold broadband enhancement in photon extraction efficiency.
- Application Focus: Optimized for optically addressable defect qubits, specifically near-surface NV centers (100 nm depth) created via implantation and annealing.
- Design Methodology: Utilized topology optimization (inverse design) via 3D FDFD solvers to tailor spectral response and collection mode, while incorporating fabrication constraints (e.g., minimum feature size of 50 nm).
- Material Stack: Hybrid structure consisting of a 250 nm thick GaP membrane (high index, n = 3.31) patterned onto a high-purity Single Crystal Diamond (SCD) substrate.
- Scalability: The small device footprint (1.5 ”m x 1.5 ”m) is compatible with scalable integration and on-chip electrodes for frequency tuning.
- Stability Improvement: Post-fabrication oxygen annealing at 400 °C was shown to significantly improve NV charge state stability (NV-/NV0 ratio) and reduce spectral diffusion, addressing key challenges in near-surface qubit integration.
Technical Specifications
Section titled âTechnical Specificationsâ| Parameter | Value | Unit | Context |
|---|---|---|---|
| Maximum PL Enhancement (Measured) | 14 | -fold | Broadband ZPL enhancement (575 nm to 750 nm) |
| Simulated PL Enhancement (z-dipole) | 15.7 | -fold | Relative to bare diamond-air interface (100 nm depth) |
| Absolute Collection Efficiency (Optimized) | 20 | % | Simulated total NV radiation collected |
| NV Center Target Depth | 100 ± 20 | nm | Below diamond surface (Implanted 15N at 85 keV) |
| GaP Refractive Index (n) | 3.31 | - | At NV emission energy (low loss) |
| GaP Membrane Thickness | 250 | nm | Transferred layer thickness |
| Device Footprint (Lateral) | 1.5 x 1.5 | ”m2 | Inverse-designed extractor structure |
| NV ZPL Wavelength (Negative Charge) | 637 | nm | Optimization target frequency |
| Initial Annealing Temperature (Sample B) | 1200 | °C | CVD diamond, 15N implantation |
| Post-Fabrication Annealing | 400 | °C | Oxygen flow, 4 hours (for stability improvement) |
| Minimum Feature Size (Design Constraint) | 50 | nm | Restricted by Electron Beam Lithography (EBL) |
| Single NV Linewidth (Post-Anneal, Device) | 844 | MHz | Average device-coupled NV linewidth |
Key Methodologies
Section titled âKey MethodologiesâThe photon extractors were designed and fabricated using advanced nanophotonic and material processing techniques:
- Inverse Design Optimization: Topology optimization (TO) was employed using a 3D Finite-Difference Frequency-Domain (FDFD) solver, maximizing the minimum Poynting flux (t) through a collection surface 0.4 ”m above the device, ensuring robustness across different dipole polarizations (x, y, z).
- Material Preparation: High-purity Single Crystal Diamond (SCD) substrates (HPHT and CVD electronic grade) were used. NV centers were created via 14N or 15N ion implantation (20 keV or 85 keV) followed by high-temperature vacuum annealing (800 °C or 1200 °C).
- Hybrid Stack Formation: A 250 nm thick Gallium Phosphide (GaP) membrane was transferred onto the diamond substrate using a wet lift-off process, forming the high-index dielectric layer.
- Nanofabrication: Electron Beam Lithography (EBL, 100 kV) was used to pattern the 1.5 ”m x 1.5 ”m structures in a thin HSQ resist layer. A conductive Au+Pd layer was sputtered to mitigate charging on the non-conductive diamond substrate during EBL.
- Pattern Transfer: Subsequent plasma Reactive Ion Etching (RIE) using Ar/Cl2/N2 chemistry transferred the pattern into the GaP layer, achieving near-vertical (88°) sidewalls.
- Qubit Stability Enhancement: Post-fabrication oxygen annealing at 400 °C was performed to modify the diamond surface termination, resulting in a significant increase in the desired NV-/NV0 charge state ratio and reduced spectral diffusion.
6CCVD Solutions & Capabilities
Section titled â6CCVD Solutions & CapabilitiesâThe research highlights the critical need for ultra-high purity, precisely engineered diamond substrates and advanced integration capabilities to realize scalable defect qubit arrays. 6CCVD is uniquely positioned to supply the foundational SCD materials and processing services required to replicate and advance this work.
| Applicable Materials & Services | 6CCVD Capability Match | Research Application & Advantage |
|---|---|---|
| Single Crystal Diamond (SCD) Substrates | Electronic Grade SCD: N < 5 ppb, B < 1 ppb (matching Sample B purity). Available in <100> orientation up to 10 mm thick. | Provides the ultra-low defect density necessary for high optical coherence and long spin coherence times in NV centers. |
| Custom Dimensions & Scalability | Large-Format PCD/SCD: Wafers up to 125 mm (PCD) and plates up to 10x10 mm (SCD). Substrates up to 10 mm thick. | Supports the transition from small-scale research arrays (2 mm x 2 mm) to high-volume, wafer-scale fabrication of quantum devices. |
| Surface Preparation & Polishing | Precision Polishing: SCD surfaces polished to Ra < 1 nm. | Essential for minimizing surface strain and defects prior to GaP membrane transfer, directly addressing the spectral diffusion and strain issues observed at the GaP-diamond interface. |
| Integration Support (Implantation Depth) | Custom Thickness Control (0.1 ”m - 500 ”m): 6CCVD provides precisely controlled SCD layer thicknesses, facilitating the required pre-implantation etching or surface preparation for accurate 100 nm NV depth placement. | Ensures optimal coupling between the near-surface NV centers and the inverse-designed photonic mode. |
| Integrated Circuitry & Tuning | Custom Metalization: In-house deposition of Au, Pt, Pd, Ti, W, Cu. | Enables the integration of on-chip electrodes for dynamic Stark tuning and frequency control, which is necessary to bridge the observed static inhomogeneity (30 ± 15 GHz blue shift) between coupled NV centers. |
| Engineering Support | In-house PhD Material Science Team: Consultation on material selection, surface termination optimization (e.g., post-annealing recipes), and strain mitigation for similar quantum emitter projects. | Assists researchers in optimizing the critical post-fabrication steps (like the 400 °C oxygen anneal) to maximize NV charge state stability and reduce the 844 MHz linewidth observed in device-coupled NVs. |
For custom specifications or material consultation, visit 6ccvd.com or contact our engineering team directly.
View Original Abstract
Solid-state defect qubit systems with spin-photon interfaces show great promise for quantum information and metrology applications. Photon collection efficiency, however, presents a major challenge for defect qubits in high refractive index host materials. Inverse-design optimization of photonic devices enables unprecedented flexibility in tailoring critical parameters of a spin-photon interface including spectral response, photon polarization, and collection mode. Further, the design process can incorporate additional constraints, such as fabrication tolerance and material processing limitations. Here, we design and demonstrate a compact hybrid gallium phosphide on diamond inverse-design planar dielectric structure coupled to single near-surface nitrogen-vacancy centers formed by implantation and annealing. We observe up to a 14-fold broadband enhancement in photon extraction efficiency, in close agreement with simulations. We expect that such inverse-designed devices will enable realization of scalable arrays of single-photon emitters, rapid characterization of new quantum emitters, efficient sensing, and heralded entanglement schemes.