2003
DOI: 10.1098/rsta.2003.1209
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Oxford ion-trap quantum computing project

Abstract: We describe recent progress in the development of an ion-trap quantum information processor. We discuss the choice of ion species and describe recent experiments on read-out for a ground-state qubit and photoionization trap loading.

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Cited by 16 publications
(7 citation statements)
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“…However, it should not be forgotten that it is often heating rate, ṅ, and not the noise per se, which is of interest for many trapped-ion applications. There are, obviously, many considerations which go into selection of ion species to be used (Jefferts et al, 1998;Wineland et al, 2003;Lucas et al, 2003). One aspect which may be added to the list of considerations is that the heating rate is inversely proportional to the ion mass.…”
Section: A Reduction Of Noisementioning
confidence: 99%
“…However, it should not be forgotten that it is often heating rate, ṅ, and not the noise per se, which is of interest for many trapped-ion applications. There are, obviously, many considerations which go into selection of ion species to be used (Jefferts et al, 1998;Wineland et al, 2003;Lucas et al, 2003). One aspect which may be added to the list of considerations is that the heating rate is inversely proportional to the ion mass.…”
Section: A Reduction Of Noisementioning
confidence: 99%
“…Moreover, channels for the delivery of atoms or ions into the cavity and the integration of trapping structures into the cavity may impose further constraints on the cavity length. In the case of ion-trap quantum computing [9], the dielectric mirrors forming the cavity can also distort the radio-frequency fields required for trapping the ion due to their electric susceptibility and due to surface charges if they are too close to the trap electrodes [10,11].…”
Section: Introductionmentioning
confidence: 99%
“…Strong coupling between emitter and cavity photon can be realized by a small cavity volume and therefore by a very short optical cavity. However, for many realistic quantum setups the cavity mirrors cannot be placed too close to each other due to technical difficulties: for trapped ion systems, short cavities lead to electrical charging of the dielectric mirrors and to distortion of the radio frequency ion trapping fields [7]; for neutral atoms, short cavity lengths are limited by the requirement for delivery of atoms into the cavity and for optical side access [8,9] for cooling and trapping. Thus, optical cavities utilized in quantum optical device applications need to combine a strong coupling rate with low losses while keeping the mirrors sufficiently apart.…”
Section: Introductionmentioning
confidence: 99%