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Bulletin of the American Physical Society

Coherence Investigations of Erbium doped in Waveguide Structures for a Quantum Memory

M. U. Staudt, Sara R. Hastings-Simon, Björn Lauritzen, Mikael Afzelius, Hugues de Riedmatten, Nicolas Sangouard, Ch. Simon, Wolfgang Tittel, Nicolas Gisin

Published Mar 7, 2007• 0 citations
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Erbium-167-doped yttrium orthosilicate is an ideal candidate for a microwave-addressed quantum memory due to its telecom wavelength optical transition and hyperfine structure with and without an applied magnetic field. However, to date there has been little investigation in coherence times for transitions around zero magnetic field, or for hyperfine structure other than from the ground state. Through the use of Raman heterodyne spectroscopy, we have identified transitions at zero magnetic field with a small dependence on field that are suitable for detecting spin echoes for both the ground and excited state. We measured coherence times of transitions at 879.4 MHz and 896.7 MHz as 370 $\mu$s and 1.4 ms respectively at 3.2 K. This is a 100-fold increase in coherence time compared to previous measurements at the same dopant concentration and 200 times greater than the even isotopes of erbium-doped yttrium orthosilicate previously used to demonstrate a microwave memory.

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Spin echoes in the ground and an optically excited state of 167^{167}167Er3+^{3+}3+:Y2_22​SiO5_55​ at near-zero magnetic fields using Raman heterodyne spectroscopy
Erbium-167-doped yttrium orthosilicate is an ideal candidate for a microwave-addressed quantum memory due to its telecom wavelength optical transition and hyperfine structure with and without an applied magnetic field. However, to date there has been little investigation in coherence times for transitions around zero magnetic field, or for hyperfine structure other than from the ground state. Through the use of Raman heterodyne spectroscopy, we have identified transitions at zero magnetic field with a small dependence on field that are suitable for detecting spin echoes for both the ground and excited state. We measured coherence times of transitions at 879.4 MHz and 896.7 MHz as 370 μ\muμs and 1.4 ms respectively at 3.2 K. This is a 100-fold increase in coherence time compared to previous measurements at the same dopant concentration and 200 times greater than the even isotopes of erbium-doped yttrium orthosilicate previously used to demonstrate a microwave memory.