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Bulletin of the American Physical Society

Optically Active Erbium with Co-dopants in Silicon

Sufian M. Abedrabbo, Abderrahmane Manu Haddad, K. Albath, Q. Younis, A. T. Fiory, Nuggehalli M. Ravindra

Published Mar 11, 2008• 0 citations
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Advanced Optical Materials•May 1, 2024•0 citations
Abstract The integration of coherent emitters into low‐loss photonic circuits is a key technology for quantum networking. In this context, nanophotonic silicon devices implanted with erbium are a promising hardware platform that combines advanced wafer‐scale nanofabrication technology with coherent emission in the minimal‐loss band of optical fibers. Recent studies have reported two distinct sites in the silicon lattice in which erbium can be reproducibly integrated with particularly promising properties. Here, for an in‐depth analysis of these sites, resonant fluorescence spectroscopy is performed on a nanophotonic waveguide in magnetic fields applied along different orientations. In this way, the site symmetry is determined, the spin Hamiltonian is reconstructed and a partial fit of the crystal field Hamiltonian is performed. The obtained quantitative description of the magnetic interaction allows the optimization of Zeeman splittings, optical branching ratios or microwave driving to the needs of future experiments. Beyond that, the derived site symmetry constrains the location of the erbium dopant in the silicon unit cell. This is a key step toward a detailed microscopic understanding of the erbium sites, which may help to improve the integration yield, thus paving the way to efficient nanophotonic quantum memories based on the Er:Si platform.
Spectral Multiplexing of Rare-Earth Emitters Individual erbium dopant atoms (yellow) in crystals made from other elements can be detected by measuring fluorescence light after resonant excitation with a laser. When the dopants are located at a site that is neighboring another dopant atom (blue), the resonance frequency is changed because of the mutual interaction. This allows one to tailor the spectral distribution of the emitters even at very low concentrations, such that correspondingly co-doped crystals can be better used for quantum information applications. For further details, see article number 2302897 by Andreas Reiserer and co-workers. [Cover image by C. Hohmann, MCQST.]