Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Bulletin of the American Physical Society

Spin-photon interface and spin-controlled photon switching in a nanobeam waveguide

Peter Lodahl

Published Mar 4, 2019• 0 citations
OpenAlex

Related papers

Spin–photon interface and spin-controlled photon switching in a nanobeam waveguide

Alisa Javadi, Dapeng Ding, Martin Hayhurst Appel +13 more

arXiv:1709.06369•Nature Nanotechnology•Mar 19, 2018•114 citations

Nanodiamond deposited on waveguides for a spin-photon interface

Joe A. Smith, John Rarity, Jake Kennard +2 more

•Jan 1, 2016•0 citations

Controlling spin-photon interfaces and nuclear spin registers in color centers

Sophia E. Economou

Bulletin of the American Physical Society•Jun 2, 2020•0 citations

Spin-Photon Interface Controlled Optical Switching in a Nanobeam Waveguide

Tim Schröder, Alisa Javadi, Dapeng Ding +13 more

We demonstrate a single InGaAs quantum dot electron spin controlled photon switch in a nanobeam waveguide with 4-fold switching ratio, a spin-state preparation fidelity of 96%, and a lifetime T1 approaching 5 µs.

Conference on Lasers and Electro-Optics•Jan 1, 2018•0 citations

Inverse-Designed Nanobeam Cavities for High-Cooperativity Spin-Photon Interfaces in Silicon

Nail Letty, Md Sakibul Islam, Wayesh Qarony

Telecom-band spin defects in silicon offer a compelling platform for integrated quantum networks by combining scalable silicon photonics with spin-based quantum memories and multiqubit registers. The T center and recently demonstrated Al1 center are particularly promising, but their limited coherent zero-phonon emission requires strong cavity enhancement for efficient spin-photon interfaces. Here, we inverse-design silicon nanobeam cavities for both centers using a unified adjoint-optimization framework targeting Purcell enhancement, resonance alignment, and photon extraction. For each emitter, symmetric cavities maximize Purcell enhancement, while asymmetric cavities provide directional coupling to an integrated waveguide. Three-dimensional finite-difference time-domain simulations yield loaded quality factors up to 3.25 x 10^6, Purcell factors up to 1.43 x 10^5, and cooperativities of approximately 280-5000, corresponding to cavity-coupled emission fractions exceeding 99.6%. The asymmetric cavities direct approximately 90% of emitted power into a single on-chip waveguide while maintaining cooperativity above 280. Under nanometer-scale fabrication perturbations, all four designs remain within the high-cooperativity regime, and high cooperativity persists when the cavity quality factor is constrained to a realistic absorption-limited value of 10^5. This unified, fabrication-compatible framework establishes a scalable cavity-design route for silicon telecom spin-photon interfaces and, to our knowledge, the first cavity designs for the Al1 center.

quant-pharXiv:2609.32205•Sep 29, 2026

Progress towards a spin photon interface

Felipe Ortiz Huerta

•Jan 1, 2016•0 citations
Telecom-band spin defects in silicon offer a compelling platform for integrated quantum networks by combining scalable silicon photonics with spin-based quantum memories and multiqubit registers. The T center and recently demonstrated Al1 center are particularly promising, but their limited coherent zero-phonon emission requires strong cavity enhancement for efficient spin-photon interfaces. Here, we inverse-design silicon nanobeam cavities for both centers using a unified adjoint-optimization framework targeting Purcell enhancement, resonance alignment, and photon extraction. For each emitter, symmetric cavities maximize Purcell enhancement, while asymmetric cavities provide directional coupling to an integrated waveguide. Three-dimensional finite-difference time-domain simulations yield loaded quality factors up to 3.25 x 10^6, Purcell factors up to 1.43 x 10^5, and cooperativities of approximately 280-5000, corresponding to cavity-coupled emission fractions exceeding 99.6%. The asymmetric cavities direct approximately 90% of emitted power into a single on-chip waveguide while maintaining cooperativity above 280. Under nanometer-scale fabrication perturbations, all four designs remain within the high-cooperativity regime, and high cooperativity persists when the cavity quality factor is constrained to a realistic absorption-limited value of 10^5. This unified, fabrication-compatible framework establishes a scalable cavity-design route for silicon telecom spin-photon interfaces and, to our knowledge, the first cavity designs for the Al1 center.