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Conference on Lasers and Electro-Optics

In-Situ Single-Photon Detection of Er Sites in Si

Ian R. Berkman, Alexey Lyasota, Gabriele G. de Boo, John G. Bartholomew, Brett C. Johnson, Jeffrey Colin McCallum, Bin-Bin Xu, Shouyi Xie, Rose L. Ahlefeldt, Matthew J. Sellars, Chunming Yin, Sven M. J. Rogge

Published Jan 1, 2022• 0 citations
Publisher

Abstract

Using sample-on-SSPD and photoluminescence excitation spectroscopy, we demonstrate Er sites in Si with inhomogeneous broadening below 100 MHz, a 350 kHz upper bound on the homogeneous linewidth, and electron T1 lower bound of 1 second.
DOI
10.1364/cleo_qels.2022.fm5d.5

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Photoluminescence of Er 3+ ions in amorphous silicon layers under intensive laser excitation

Boris V. Kamenev, Vladimir I Emel'yanov, Константинова Елизавета Александровна +5 more

Applied Physics B•Feb 1, 2002•5 citations
We present a flexible method to study the optical properties of an Er3+{\mathrm{Er}}^{3+}Er3+ ensemble in Si\mathrm{Si}Si accessed via resonant excitation and in situ single-photon detection. The technique allows an efficient resonant photoluminescence detection of optically active centers with weak oscillator strength in transparent crystals without the need for nanofabrication on the sample. We observe 70 Er3+{\mathrm{Er}}^{3+}Er3+ resonances in Si\mathrm{Si}Si, of which 62 resonances have not been observed in the literature, with optical lifetimes ranging from 0.5 to 1.5 ms. We observe inhomogeneous broadening of less than 400 MHz and an upper bound on the homogeneous linewidth of 0.75 and 1.4 MHz for two separate resonances. These narrow, stable resonances confirm Er3+{\mathrm{Er}}^{3+}Er3+ in Si\mathrm{Si}Si as a promising quantum information candidate. We discuss the use of this technique for rapid characterization of future samples, with the aim of enhancing the prevalence of sites which are favorable for quantum information applications.
Rare-earth ions in solid-state hosts exhibit low homogeneous broadening and long spin coherence at cryogenic temperatures thus making them a promising candidate for optical quantum memories [1], optical-microwave transducers [2] and single dopant-based devices such as single photon emitters operating at the telecommunication wavelengths [3]. Here, we present an overview of the spin and optical properties of Er ensembles in Si accessed via resonant photoluminescence excitation (PLE) spectroscopy [4]. Samples were positioned directly on top of tailor-fabricated superconducting single photon detectors, placed in a dilution refrigerator unit and resonantly excited using fiber optics. Our method provided high collection efficiency and allowed spectral measurements of low Er density samples. The observed Er PLE spectra were strongly affected by the presence of co-dopants such as O, B or P reflecting their influence on the formation of optically active Er sites and corresponding Er optical transition energies. Higher O densities resulted in especially rich PLE spectra suggesting that a variety of Er-O complexes formed due to O doping. Lowering the O concentration, we achieved PLE spectra dominated by a single Er site in P doped samples. Interestingly, the Er spin relaxation and optical coherence properties were barely affected by the employed co-dopants and mainly depended on the Er concentration. By lowering the Er concentration from relatively high (1018cm-3) to low densities (1016cm-3), we were able to increase Er spin lifetimes from ~0.1 s to ~30 s. Long spin relaxation times allowed us to identify PLE spectra of new Er sites in Si. In both concentration regimes, we observed sub-MHz transient spectral holes suggesting long optical coherence times. Furthermore, we observed sub-MHz spin transitions in both natural and isotopically purified Si and achieved spin coherence times above 1 ms in isotopically purified Si. Narrow optical linewidths and long transverse and longitudinal spin relaxation times show that Er in Si is an excellent candidate for future quantum information and communication applications.
We present the results of detailed site-selective spectroscopy performed on the $^{4}I_{15∕2}\ensuremath{\leftrightarrow}^{4}I_{13∕2}$ transition of Er3+:Y2SiO5{\mathrm{Er}}^{3+}:{\mathrm{Y}}_{2}\mathrm{Si}{\mathrm{O}}_{5}Er3+:Y2​SiO5​ at $1.5\phantom{\rule{0.3em}{0ex}}\ensuremath{\mu}\mathrm{m}$. New determinations of the 4I13∕2^{4}I_{13∕2}4I13∕2​ and 4I15∕2^{4}I_{15∕2}4I15∕2​ crystal-field-level structure for the two crystallographically inequivalent Er3+{\mathrm{Er}}^{3+}Er3+ sites have been made. The fluorescence dynamics of the metastable 4I13∕2:Y1^{4}I_{13∕2}:{\mathrm{Y}}_{1}4I13∕2​:Y1​ excited state was investigated, showing exponential decays for Er3+{\mathrm{Er}}^{3+}Er3+ at both crystallographic sites with fluorescence lifetimes of 11.4ms11.4\phantom{\rule{0.3em}{0ex}}\mathrm{ms}11.4ms for site 1 and 9.2ms9.2\phantom{\rule{0.3em}{0ex}}\mathrm{ms}9.2ms for site 2. Exceptionally sharp inhomogeneous absorption lines of 180, 390, and 510MHz510\phantom{\rule{0.3em}{0ex}}\mathrm{MHz}510MHz were observed in 0.0015% Er3+:Y2SiO5{\mathrm{Er}}^{3+}:{\mathrm{Y}}_{2}\mathrm{Si}{\mathrm{O}}_{5}Er3+:Y2​SiO5​, 0.005% Er3+:Y2SiO5{\mathrm{Er}}^{3+}:{\mathrm{Y}}_{2}\mathrm{Si}{\mathrm{O}}_{5}Er3+:Y2​SiO5​, and 0.02% Er3+:Y2SiO5{\mathrm{Er}}^{3+}:{\mathrm{Y}}_{2}\mathrm{Si}{\mathrm{O}}_{5}Er3+:Y2​SiO5​ crystals, respectively. The ggg-values for the lowest energy 4I15∕2^{4}I_{15∕2}4I15∕2​ (Z1)({\mathrm{Z}}_{1})(Z1​) and 4I13∕2^{4}I_{13∕2}4I13∕2​ (Y1)({\mathrm{Y}}_{1})(Y1​) doublets were measured to be 5.5 and 4.6 for site 1 and 15.0 and 12.9 for site 2 when the magnetic field was oriented along the crystal's ${\mathbit{D}}_{1}$ axis.