TY - JOUR
T1 - Room-temperature 1.54 µm photoluminescence of Er:Ox centers at extremely low concentration in silicon
AU - Celebrano, Michele
AU - Ghirardini, Lavinia
AU - Biagioni, Paolo
AU - Finazzi, Marco
AU - Shimizu, Yasuo
AU - Tu, Yuan
AU - Inoue, Koji
AU - Nagai, Yasuyoshi
AU - Shinada, Takahiro
AU - Chiba, Yuki
AU - Abdelghafar, Ayman
AU - Yano, Maasa
AU - Tanii, Takashi
AU - Prati, Enrico
N1 - Publisher Copyright:
Copyright © 2017, The Authors. All rights reserved.
Copyright:
Copyright 2020 Elsevier B.V., All rights reserved.
PY - 2017/2/1
Y1 - 2017/2/1
N2 - The demand for single photon sources at λ = 1.54 µm, which follows from the consistent development of quantum networks based on commercial optical fibers, makes Er:Ox centers in Si still a viable resource thanks to the optical transition of Er3+: 4I13/2 → 4I15/2. Yet, to date, the implementation of such system remains hindered by its extremely low emission rate. In this Letter, we explore the room-temperature photoluminescence (PL) at the telecomm wavelength of very low implantation doses of Er:Ox in Si. The emitted photons, excited by a λ = 792 nm laser in both large areas and confined dots of diameter down to 5 µm, are collected by an inverted confocal microscope. The lower-bound number of detectable emission centers within our diffraction-limited illumination spot is estimated to be down to about 104, corresponding to an emission rate per individual ion of about 4 ×103 photons/s.
AB - The demand for single photon sources at λ = 1.54 µm, which follows from the consistent development of quantum networks based on commercial optical fibers, makes Er:Ox centers in Si still a viable resource thanks to the optical transition of Er3+: 4I13/2 → 4I15/2. Yet, to date, the implementation of such system remains hindered by its extremely low emission rate. In this Letter, we explore the room-temperature photoluminescence (PL) at the telecomm wavelength of very low implantation doses of Er:Ox in Si. The emitted photons, excited by a λ = 792 nm laser in both large areas and confined dots of diameter down to 5 µm, are collected by an inverted confocal microscope. The lower-bound number of detectable emission centers within our diffraction-limited illumination spot is estimated to be down to about 104, corresponding to an emission rate per individual ion of about 4 ×103 photons/s.
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