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

Elsevier eBooks

Chapter 151 Coherent emission in rare-earth materials

Francois E. Auzel

Published Jan 1, 1996• 1 citation
Publisher
DOI
10.1016/s0168-1273(96)22008-2

Related papers

Coherent emission from rare-earth ions in electrooptic crystals

L. F. Johnson, A. A. Ballman

IEEE Journal of Quantum Electronics•May 1, 1968•5 citations

Recent progress in developing new rare earth materials for hole burning and coherent transient applications

Yazhou Sun, Charles W. Thiel, R. L. Cone +2 more

Journal of Luminescence•Jul 1, 2002•210 citations

Epitaxial rare-earth quantum material and devices (Conference Presentation)

Tian Zhong

Coherent quantum devices play a central role in quantum science and engineering. Rare-earth ions such as erbium in solids feature numerous 4f- intra-shell transitions that are effectively shielded from their crystalline surroundings by closed outer shells, allowing for long spin coherence times and narrow optical transitions. Recent ensemble experiments have established the rare-earth doped crystals as the leading materials for optical quantum memories. However, the development of large-scale quantum devices based on rare-earth doped materials has remained a challenge. Here we describe a scalable quantum photonic platform based on epitaxially grown oxide thin films doped with trivalent ions on silicon substrates. The platform builds upon the recent developments of high quality epitaxial rare-earth doped oxides on silicon, and highlights the integration of quantum coherent materials with existing silicon technologies for ultimate device scalability. The proposed device platform builds upon our capability to epitaxially grow high quality, near-lattice-matched Y2O3 thin films on silicon. The epitaxial thin film is of high structural quality and offers several distinct advantages: (1) significantly less optical loss and better quantum emitter coherence; (2) atomic precision placement of rare-earth emitters (via delta doping) with respect to the photonic mode for controllable ion-photon coupling; (3) scalable top-down device fabrication using standard lithography and etching techniques; (4) heterogeneous integration with silicon takes full advantage of existing silicon photonics technologies for routing, tuning, and modulation of the quantum emission from rare-earth ions.

Quantum Nanophotonic Materials, Devices, and Systems•Sep 10, 2019•0 citations

Absorption and Emission in Rare Earths

WORLD SCIENTIFIC eBooks•Nov 17, 2014•0 citations

UNCONVENTIONAL LIGHT EMISSIONS IN RARE-EARTH DOPED SOLIDS

Francois E. Auzel

•Nov 1, 2001•0 citations

Deactivation of the photoionization excitation mechanism of rare-earth intraion emission in ZnS

Krzysztof Swiatek, M. Godlewski

A new, very efficient excitation mechanism of the rare-earth (RE) intraion emission was observed recently. This is a process in which the RE ion undergoes ionization and the RE intraion emission is induced when the ionized carrier is recaptured by the RE. The capture process proceeds via an intermediate state due to RE bound exciton (BE), from which the energy is transferred to the RE excited state. In this letter we discuss mechanisms which limit the efficiency of this excitation channel. The first is the thermal dissociation of the RE BE, which reduces the efficiency of the energy transfer thus quenches the RE intraion emission. It is also indicated that an efficient energy transfer from RE Be to iron Fe2+ centers competes with the transfer of the BE energy to RE core states. Our results mean that the practical utilization of the above excitation mechanism of emission in the RE-activated ZnS devices may be hampered by the common contamination of this material with iron.

Applied Physics Letters•May 28, 1990•14 citations
Coherent quantum devices play a central role in quantum science and engineering. Rare-earth ions such as erbium in solids feature numerous 4f- intra-shell transitions that are effectively shielded from their crystalline surroundings by closed outer shells, allowing for long spin coherence times and narrow optical transitions. Recent ensemble experiments have established the rare-earth doped crystals as the leading materials for optical quantum memories. However, the development of large-scale quantum devices based on rare-earth doped materials has remained a challenge. Here we describe a scalable quantum photonic platform based on epitaxially grown oxide thin films doped with trivalent ions on silicon substrates. The platform builds upon the recent developments of high quality epitaxial rare-earth doped oxides on silicon, and highlights the integration of quantum coherent materials with existing silicon technologies for ultimate device scalability. The proposed device platform builds upon our capability to epitaxially grow high quality, near-lattice-matched Y2O3 thin films on silicon. The epitaxial thin film is of high structural quality and offers several distinct advantages: (1) significantly less optical loss and better quantum emitter coherence; (2) atomic precision placement of rare-earth emitters (via delta doping) with respect to the photonic mode for controllable ion-photon coupling; (3) scalable top-down device fabrication using standard lithography and etching techniques; (4) heterogeneous integration with silicon takes full advantage of existing silicon photonics technologies for routing, tuning, and modulation of the quantum emission from rare-earth ions.
A new, very efficient excitation mechanism of the rare-earth (RE) intraion emission was observed recently. This is a process in which the RE ion undergoes ionization and the RE intraion emission is induced when the ionized carrier is recaptured by the RE. The capture process proceeds via an intermediate state due to RE bound exciton (BE), from which the energy is transferred to the RE excited state. In this letter we discuss mechanisms which limit the efficiency of this excitation channel. The first is the thermal dissociation of the RE BE, which reduces the efficiency of the energy transfer thus quenches the RE intraion emission. It is also indicated that an efficient energy transfer from RE Be to iron Fe2+ centers competes with the transfer of the BE energy to RE core states. Our results mean that the practical utilization of the above excitation mechanism of emission in the RE-activated ZnS devices may be hampered by the common contamination of this material with iron.