Implanted SiV Centers in Diamond for Spectral Stability
Find Innovative SolutionsGenerate Solutions
Solution Overview
Problem
Current quantum information systems face challenges in combining high brightness and narrowband emission with low inhomogeneous photon frequency distribution, particularly in integrating spectrally stable emitters into nanophotonic structures, due to the sensitivity of nitrogen-vacancy (NV−) centers to their local environment.
Innovation Solution
The use of implanted silicon-vacancy (SiV−) and germanium-vacancy (GeV−) centers in diamond, created through ion implantation and high-temperature annealing, which exhibit nearly lifetime-limited optical linewidths and a narrow inhomogeneous distribution, allowing for deterministic placement in nanophotonic devices.
Engineering Contradictions & Design Principles
Engineering Contradiction Analysis
1Illumination intensity
If nitrogen-vacancy (NV−) centers are used as quantum emitters, then high brightness and photostability are achieved, but spectral stability deteriorates due to sensitivity to local environment
Solution Approach 1:
The patent transitions from NV− centers to SiV− centers, changing the chemical composition parameter of the defect. SiV− centers have different electronic structure and symmetry properties that inherently provide immunity to Stark shifts, thus achieving spectral stability while maintaining brightness
2Ease of manufacture
If semiconductor quantum dots are used as quantum emitters, then ease of integration into nanophotonic structures is achieved, but inhomogeneous distribution of photon frequencies worsens
Solution Approach 1:
The patent employs focused ion beam implantation to create SiV− centers at specific predetermined locations within the diamond lattice. This localized defect creation method ensures precise spatial positioning and uniform spectral properties, achieving both ease of integration and low inhomogeneous distribution
Solution Approach 2:
The patent performs defect engineering through ion implantation and thermal annealing before nanofabrication. By pre-establishing SiV− centers with controlled positions and spectral properties, the subsequent integration into nanophotonic structures becomes straightforward while maintaining uniform emission characteristics
3Productivity
If NV− centers are integrated into nanophotonic structures to improve photon generation rates, then productivity is improved, but spectral stability deteriorates
Solution Approach 1:
The patent changes the defect type from NV− to SiV− centers, which have different symmetry properties. SiV− centers possess inversion symmetry that protects them from first-order Stark shifts, maintaining spectral stability even when integrated into nanophotonic structures for high-rate photon generation
Applied Scientific Principles
This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.
Function Achieved in This Case
These centers maintain their favorable optical properties after nanofabrication, enabling scalable integration into quantum nano-optical devices with improved yields and reproducibility, providing stable and indistinguishable photon sources.
Implementation Method 1
implanted silicon-vacancy (SiV−) centers in diamond
Implementation Method 2
created through ion implantation and high-temperature annealing
Data Source
AI summary
In an exemplary embodiment, a structure comprises a plurality of deterministically positioned optically active defects, wherein each of the plurality of deterministically positioned optically active defects has a linewidth within a factor of one hundred of a lifetime limited linewidth of optical transitions of the plurality of deterministically positioned optically active defects, and wherein the plurality of deterministically positioned optically active defects has an inhomogeneous distribution of wavelengths, wherein at least half of the plurality of deterministically positioned optically active defects have transition wavelengths within a less than 8 nm range. In a further exemplary embodiment, method of producing at least one optically active defect comprises deterministically implanting at least one ion in a structure using a focused ion beam; heating the structure in a vacuum at a first temperature to create at least one optically active defect; and heating the structure in the vacuum at a second temperature to remove a plurality of other defects in the structure, wherein the second temperature is higher than the first temperature.


